Section 5.4 (Systems of Linear Differential Equation); 9.5 Eigenvalues and Eigenvectors, cont d
|
|
- Rudolph McKenzie
- 5 years ago
- Views:
Transcription
1 Section 5.4 (Systems of Linear Differential Equation); 9.5 Eigenvalues and Eigenvectors, cont d July 6, 2009
2 Today s Session
3 Today s Session A Summary of This Session:
4 Today s Session A Summary of This Session: (1) More about eigenvalues and eigenvectors of a 2 2 matrix.
5 Today s Session A Summary of This Session: (1) More about eigenvalues and eigenvectors of a 2 2 matrix. (2) 2 2 systems of differential equations (not necessarily linear)
6 Today s Session A Summary of This Session: (1) More about eigenvalues and eigenvectors of a 2 2 matrix. (2) 2 2 systems of differential equations (not necessarily linear) (3) Phase-plane method (types of nodes)
7 Today s Session A Summary of This Session: (1) More about eigenvalues and eigenvectors of a 2 2 matrix. (2) 2 2 systems of differential equations (not necessarily linear) (3) Phase-plane method (types of nodes)
8 Today s Session A Summary of This Session: (1) More about eigenvalues and eigenvectors of a 2 2 matrix. (2) 2 2 systems of differential equations (not necessarily linear) (3) Phase-plane method (types of nodes)
9 Critical points, critical point set, equilibrium point(s) Example 1: Consider the system: x = x y y = x + y 2
10 Critical points, critical point set, equilibrium point(s) Example 1: Consider the system: x = x y y = x + y 2 Find the critical point(s), eigenvalues and eigenvectors, and describe completely the solution set.
11 Critical points, critical point set, equilibrium point(s) Example 1: Consider the system: x = x y y = x + y 2 Find the critical point(s), eigenvalues and eigenvectors, and describe completely the solution set. To find the critical points, one needs to solve, simultaneously, x = 0 y = 0
12 Critical points, critical point set, equilibrium point(s) Example 1: Consider the system: x = x y y = x + y 2 Find the critical point(s), eigenvalues and eigenvectors, and describe completely the solution set. To find the critical points, one needs to solve, simultaneously, This means: x = 0 y = 0 x y = 0 x + y 2 = 0
13 Critical points, critical point set, equilibrium point(s) Example 1: Consider the system: x = x y y = x + y 2 Find the critical point(s), eigenvalues and eigenvectors, and describe completely the solution set. To find the critical points, one needs to solve, simultaneously, This means: So the critical point is (1,1). x = 0 y = 0 x y = 0 x + y 2 = 0
14 Example 1: Case of a Spiral To find the eigenvalues, we first put the system in the form v = A v + v 0 Where ( ) ( ) x 1 1 v =, A =, and ( ) 0 v y =. Note 2 the book (in section 9.5) uses x for the vector v. The eigenvalues of A are: λ = 1 ± i. This means the node (1,1) is an unstable spiral. Graph this on pplane.
15 Example 2: Case of an Asymptotically Stable Node (Stable Spiral) Consider the system: x = x 2y + 2 y = 8x y + 1
16 Example 2: Case of an Asymptotically Stable Node (Stable Spiral) Consider the system: x = x 2y + 2 y = 8x y + 1 Find the critical point(s), eigenvalues and eigenvectors, and describe completely the solution set.
17 Example 2: Case of an Asymptotically Stable Node (Stable Spiral) Consider the system: x = x 2y + 2 y = 8x y + 1 Find the critical point(s), eigenvalues and eigenvectors, and describe completely the solution set. To find the critical points, one needs to solve, simultaneously, x = 0 y = 0
18 Example 2: Case of an Asymptotically Stable Node (Stable Spiral) Consider the system: x = x 2y + 2 y = 8x y + 1 Find the critical point(s), eigenvalues and eigenvectors, and describe completely the solution set. To find the critical points, one needs to solve, simultaneously, This means: x = 0 y = 0 x 2y = 2 8x y = 1
19 Example 2: Case of an Asymptotically Stable Node (Stable Spiral) Consider the system: x = x 2y + 2 y = 8x y + 1 Find the critical point(s), eigenvalues and eigenvectors, and describe completely the solution set. To find the critical points, one needs to solve, simultaneously, This means: So the critical point is (0,1). x = 0 y = 0 x 2y = 2 8x y = 1
20 Example 2, cont d To find the eigenvalues, we first put the system in the form v = A v + v 0 Where ( ) ( ) x 1 2 v =, A =, and ( ) 2 v y =. The 1 eigenvalues of A are: λ = 1 ± 4i. We have an asymptotically stable spiral at (0,1). Graph this in pplane.
21 Example 3: Determine the nature of nodes for x = 2x 5y y = x + 2y
22 Example 3: Determine the nature of nodes for x = 2x 5y y = x + 2y To find the critical points, one needs to solve, simultaneously, x = 0 y = 0
23 Example 3: Determine the nature of nodes for x = 2x 5y y = x + 2y To find the critical points, one needs to solve, simultaneously, x = 0 y = 0 The critical point is the origin (0,0).
24 Example 3, cont d To find the eigenvalues, we first put the system in the form v = A v ) ( 2 5, A = 1 2 Where ( x v = y λ = ±i. Since both eigenvalues are pure imaginary numbers. We have an center at (0,0). We have periodic orbits for trajectories. ). The eigenvalues of A are:
25 Example 3, cont d Question: Use the eigenvalues and eigenvectors to solve this system.
26 Example 3, cont d Question: Use the eigenvalues and eigenvectors to solve this system. The eigenvector associated with λ 1 = i is ( 2 + i v 1 = 1 eigenvector associated with λ 2 = i is ( 2 i v 2 = 1 solution is given by: v = c1 e it v 1 + c 2 e it v 2. ). The ). The or v = c1 e it ( 2 + i 1 ) + c 2 e it ( 2 i 1 ).
Math 3301 Homework Set Points ( ) ( ) I ll leave it to you to verify that the eigenvalues and eigenvectors for this matrix are, ( ) ( ) ( ) ( )
#7. ( pts) I ll leave it to you to verify that the eigenvalues and eigenvectors for this matrix are, λ 5 λ 7 t t ce The general solution is then : 5 7 c c c x( 0) c c 9 9 c+ c c t 5t 7 e + e A sketch of
More information+ i. cos(t) + 2 sin(t) + c 2.
MATH HOMEWORK #7 PART A SOLUTIONS Problem 7.6.. Consider the system x = 5 x. a Express the general solution of the given system of equations in terms of realvalued functions. b Draw a direction field,
More informationDef. (a, b) is a critical point of the autonomous system. 1 Proper node (stable or unstable) 2 Improper node (stable or unstable)
Types of critical points Def. (a, b) is a critical point of the autonomous system Math 216 Differential Equations Kenneth Harris kaharri@umich.edu Department of Mathematics University of Michigan November
More informationMath 266: Phase Plane Portrait
Math 266: Phase Plane Portrait Long Jin Purdue, Spring 2018 Review: Phase line for an autonomous equation For a single autonomous equation y = f (y) we used a phase line to illustrate the equilibrium solutions
More informationOutline. Learning Objectives. References. Lecture 2: Second-order Systems
Outline Lecture 2: Second-order Systems! Techniques based on linear systems analysis! Phase-plane analysis! Example: Neanderthal / Early man competition! Hartman-Grobman theorem -- validity of linearizations!
More information1 The relation between a second order linear ode and a system of two rst order linear odes
Math 1280 Spring, 2010 1 The relation between a second order linear ode and a system of two rst order linear odes In Chapter 3 of the text you learn to solve some second order linear ode's, such as x 00
More information1 The pendulum equation
Math 270 Honors ODE I Fall, 2008 Class notes # 5 A longer than usual homework assignment is at the end. The pendulum equation We now come to a particularly important example, the equation for an oscillating
More informationPhase portraits in two dimensions
Phase portraits in two dimensions 8.3, Spring, 999 It [ is convenient to represent the solutions to an autonomous system x = f( x) (where x x = ) by means of a phase portrait. The x, y plane is called
More informationMathQuest: Differential Equations
MathQuest: Differential Equations Geometry of Systems 1. The differential equation d Y dt = A Y has two straight line solutions corresponding to [ ] [ ] 1 1 eigenvectors v 1 = and v 2 2 = that are shown
More information4 Second-Order Systems
4 Second-Order Systems Second-order autonomous systems occupy an important place in the study of nonlinear systems because solution trajectories can be represented in the plane. This allows for easy visualization
More informationDepartment of Mathematics IIT Guwahati
Stability of Linear Systems in R 2 Department of Mathematics IIT Guwahati A system of first order differential equations is called autonomous if the system can be written in the form dx 1 dt = g 1(x 1,
More informationCalculus and Differential Equations II
MATH 250 B Second order autonomous linear systems We are mostly interested with 2 2 first order autonomous systems of the form { x = a x + b y y = c x + d y where x and y are functions of t and a, b, c,
More informationLinear Planar Systems Math 246, Spring 2009, Professor David Levermore We now consider linear systems of the form
Linear Planar Systems Math 246, Spring 2009, Professor David Levermore We now consider linear systems of the form d x x 1 = A, where A = dt y y a11 a 12 a 21 a 22 Here the entries of the coefficient matrix
More informationENGI Linear Approximation (2) Page Linear Approximation to a System of Non-Linear ODEs (2)
ENGI 940 4.06 - Linear Approximation () Page 4. 4.06 Linear Approximation to a System of Non-Linear ODEs () From sections 4.0 and 4.0, the non-linear system dx dy = x = P( x, y), = y = Q( x, y) () with
More informationMath 1270 Honors ODE I Fall, 2008 Class notes # 14. x 0 = F (x; y) y 0 = G (x; y) u 0 = au + bv = cu + dv
Math 1270 Honors ODE I Fall, 2008 Class notes # 1 We have learned how to study nonlinear systems x 0 = F (x; y) y 0 = G (x; y) (1) by linearizing around equilibrium points. If (x 0 ; y 0 ) is an equilibrium
More informationUnderstand the existence and uniqueness theorems and what they tell you about solutions to initial value problems.
Review Outline To review for the final, look over the following outline and look at problems from the book and on the old exam s and exam reviews to find problems about each of the following topics.. Basics
More informationUsing web-based Java pplane applet to graph solutions of systems of differential equations
Using web-based Java pplane applet to graph solutions of systems of differential equations Our class project for MA 341 involves using computer tools to analyse solutions of differential equations. This
More informationMATH 215/255 Solutions to Additional Practice Problems April dy dt
. For the nonlinear system MATH 5/55 Solutions to Additional Practice Problems April 08 dx dt = x( x y, dy dt = y(.5 y x, x 0, y 0, (a Show that if x(0 > 0 and y(0 = 0, then the solution (x(t, y(t of the
More informationLecture 38. Almost Linear Systems
Math 245 - Mathematics of Physics and Engineering I Lecture 38. Almost Linear Systems April 20, 2012 Konstantin Zuev (USC) Math 245, Lecture 38 April 20, 2012 1 / 11 Agenda Stability Properties of Linear
More informationMath 308 Final Exam Practice Problems
Math 308 Final Exam Practice Problems This review should not be used as your sole source for preparation for the exam You should also re-work all examples given in lecture and all suggested homework problems
More informationMath 1280 Notes 4 Last section revised, 1/31, 9:30 pm.
1 competing species Math 1280 Notes 4 Last section revised, 1/31, 9:30 pm. This section and the next deal with the subject of population biology. You will already have seen examples of this. Most calculus
More informationSection 9.3 Phase Plane Portraits (for Planar Systems)
Section 9.3 Phase Plane Portraits (for Planar Systems) Key Terms: Equilibrium point of planer system yꞌ = Ay o Equilibrium solution Exponential solutions o Half-line solutions Unstable solution Stable
More informationMath 216 First Midterm 19 October, 2017
Math 6 First Midterm 9 October, 7 This sample exam is provided to serve as one component of your studying for this exam in this course. Please note that it is not guaranteed to cover the material that
More informationMath 331 Homework Assignment Chapter 7 Page 1 of 9
Math Homework Assignment Chapter 7 Page of 9 Instructions: Please make sure to demonstrate every step in your calculations. Return your answers including this homework sheet back to the instructor as a
More informationProblem set 6 Math 207A, Fall 2011 Solutions. 1. A two-dimensional gradient system has the form
Problem set 6 Math 207A, Fall 2011 s 1 A two-dimensional gradient sstem has the form x t = W (x,, x t = W (x, where W (x, is a given function (a If W is a quadratic function W (x, = 1 2 ax2 + bx + 1 2
More informationProblem set 7 Math 207A, Fall 2011 Solutions
Problem set 7 Math 207A, Fall 2011 s 1. Classify the equilibrium (x, y) = (0, 0) of the system x t = x, y t = y + x 2. Is the equilibrium hyperbolic? Find an equation for the trajectories in (x, y)- phase
More informationStability of critical points in Linear Systems of Ordinary Differential Equations (SODE)
Stability of critical points in Linear Systems of Ordinary Differential Equations (SODE) In this chapter Mathematica will be used to study the stability of the critical points of twin equation linear SODE.
More informationLECTURE 8: DYNAMICAL SYSTEMS 7
15-382 COLLECTIVE INTELLIGENCE S18 LECTURE 8: DYNAMICAL SYSTEMS 7 INSTRUCTOR: GIANNI A. DI CARO GEOMETRIES IN THE PHASE SPACE Damped pendulum One cp in the region between two separatrix Separatrix Basin
More informationHANDOUT E.22 - EXAMPLES ON STABILITY ANALYSIS
Example 1 HANDOUT E. - EXAMPLES ON STABILITY ANALYSIS Determine the stability of the system whose characteristics equation given by 6 3 = s + s + 3s + s + s + s +. The above polynomial satisfies the necessary
More informationCDS 101 Precourse Phase Plane Analysis and Stability
CDS 101 Precourse Phase Plane Analysis and Stability Melvin Leok Control and Dynamical Systems California Institute of Technology Pasadena, CA, 26 September, 2002. mleok@cds.caltech.edu http://www.cds.caltech.edu/
More informationStability of Dynamical systems
Stability of Dynamical systems Stability Isolated equilibria Classification of Isolated Equilibria Attractor and Repeller Almost linear systems Jacobian Matrix Stability Consider an autonomous system u
More information154 Chapter 9 Hints, Answers, and Solutions The particular trajectories are highlighted in the phase portraits below.
54 Chapter 9 Hints, Answers, and Solutions 9. The Phase Plane 9.. 4. The particular trajectories are highlighted in the phase portraits below... 3. 4. 9..5. Shown below is one possibility with x(t) and
More informationThere is a more global concept that is related to this circle of ideas that we discuss somewhat informally. Namely, a region R R n with a (smooth)
82 Introduction Liapunov Functions Besides the Liapunov spectral theorem, there is another basic method of proving stability that is a generalization of the energy method we have seen in the introductory
More informationPhase Plane Analysis
Phase Plane Analysis Phase plane analysis is one of the most important techniques for studying the behavior of nonlinear systems, since there is usually no analytical solution for a nonlinear system. Background
More informationA plane autonomous system is a pair of simultaneous first-order differential equations,
Chapter 11 Phase-Plane Techniques 11.1 Plane Autonomous Systems A plane autonomous system is a pair of simultaneous first-order differential equations, ẋ = f(x, y), ẏ = g(x, y). This system has an equilibrium
More informationB5.6 Nonlinear Systems
B5.6 Nonlinear Systems 5. Global Bifurcations, Homoclinic chaos, Melnikov s method Alain Goriely 2018 Mathematical Institute, University of Oxford Table of contents 1. Motivation 1.1 The problem 1.2 A
More informationSection 4.9; Section 5.6. June 30, Free Mechanical Vibrations/Couple Mass-Spring System
Section 4.9; Section 5.6 Free Mechanical Vibrations/Couple Mass-Spring System June 30, 2009 Today s Session Today s Session A Summary of This Session: Today s Session A Summary of This Session: (1) Free
More information8.1 Bifurcations of Equilibria
1 81 Bifurcations of Equilibria Bifurcation theory studies qualitative changes in solutions as a parameter varies In general one could study the bifurcation theory of ODEs PDEs integro-differential equations
More informationAutonomous systems. Ordinary differential equations which do not contain the independent variable explicitly are said to be autonomous.
Autonomous equations Autonomous systems Ordinary differential equations which do not contain the independent variable explicitly are said to be autonomous. i f i(x 1, x 2,..., x n ) for i 1,..., n As you
More informationMath 312 Lecture Notes Linear Two-dimensional Systems of Differential Equations
Math 2 Lecture Notes Linear Two-dimensional Systems of Differential Equations Warren Weckesser Department of Mathematics Colgate University February 2005 In these notes, we consider the linear system of
More informationLecture Notes for Math 251: ODE and PDE. Lecture 27: 7.8 Repeated Eigenvalues
Lecture Notes for Math 25: ODE and PDE. Lecture 27: 7.8 Repeated Eigenvalues Shawn D. Ryan Spring 22 Repeated Eigenvalues Last Time: We studied phase portraits and systems of differential equations with
More informationChapter 6 Nonlinear Systems and Phenomena. Friday, November 2, 12
Chapter 6 Nonlinear Systems and Phenomena 6.1 Stability and the Phase Plane We now move to nonlinear systems Begin with the first-order system for x(t) d dt x = f(x,t), x(0) = x 0 In particular, consider
More informationAutonomous Systems and Stability
LECTURE 8 Autonomous Systems and Stability An autonomous system is a system of ordinary differential equations of the form 1 1 ( 1 ) 2 2 ( 1 ). ( 1 ) or, in vector notation, x 0 F (x) That is to say, an
More informationMath Notes on sections 7.8,9.1, and 9.3. Derivation of a solution in the repeated roots case: 3 4 A = 1 1. x =e t : + e t w 2.
Math 7 Notes on sections 7.8,9., and 9.3. Derivation of a solution in the repeated roots case We consider the eample = A where 3 4 A = The onl eigenvalue is = ; and there is onl one linearl independent
More informationIn these chapter 2A notes write vectors in boldface to reduce the ambiguity of the notation.
1 2 Linear Systems In these chapter 2A notes write vectors in boldface to reduce the ambiguity of the notation 21 Matrix ODEs Let and is a scalar A linear function satisfies Linear superposition ) Linear
More information2.10 Saddles, Nodes, Foci and Centers
2.10 Saddles, Nodes, Foci and Centers In Section 1.5, a linear system (1 where x R 2 was said to have a saddle, node, focus or center at the origin if its phase portrait was linearly equivalent to one
More informationDesigning Information Devices and Systems II Fall 2015 Note 22
EE 16B Designing Information Devices and Systems II Fall 2015 Note 22 Notes taken by John Noonan (11/12) Graphing of the State Solutions Open loop x(k + 1) = Ax(k) + Bu(k) y(k) = Cx(k) Closed loop x(k
More informationModels Involving Interactions between Predator and Prey Populations
Models Involving Interactions between Predator and Prey Populations Matthew Mitchell Georgia College and State University December 30, 2015 Abstract Predator-prey models are used to show the intricate
More informationTHE SEPARATRIX FOR A SECOND ORDER ORDINARY DIFFERENTIAL EQUATION OR A 2 2 SYSTEM OF FIRST ORDER ODE WHICH ALLOWS A PHASE PLANE QUANTITATIVE ANALYSIS
THE SEPARATRIX FOR A SECOND ORDER ORDINARY DIFFERENTIAL EQUATION OR A SYSTEM OF FIRST ORDER ODE WHICH ALLOWS A PHASE PLANE QUANTITATIVE ANALYSIS Maria P. Skhosana and Stephan V. Joubert, Tshwane University
More informationMath 312 Lecture Notes Linearization
Math 3 Lecture Notes Linearization Warren Weckesser Department of Mathematics Colgate University 3 March 005 These notes discuss linearization, in which a linear system is used to approximate the behavior
More informationSample Solutions of Assignment 9 for MAT3270B
Sample Solutions of Assignment 9 for MAT370B. For the following ODEs, find the eigenvalues and eigenvectors, and classify the critical point 0,0 type and determine whether it is stable, asymptotically
More informationDi erential Equations
9.3 Math 3331 Di erential Equations 9.3 Phase Plane Portraits Jiwen He Department of Mathematics, University of Houston jiwenhe@math.uh.edu math.uh.edu/ jiwenhe/math3331 Jiwen He, University of Houston
More information2 Lyapunov Stability. x(0) x 0 < δ x(t) x 0 < ɛ
1 2 Lyapunov Stability Whereas I/O stability is concerned with the effect of inputs on outputs, Lyapunov stability deals with unforced systems: ẋ = f(x, t) (1) where x R n, t R +, and f : R n R + R n.
More informationLinear Systems of ODE: Nullclines, Eigenvector lines and trajectories
Linear Systems of ODE: Nullclines, Eigenvector lines and trajectories James K. Peterson Department of Biological Sciences and Department of Mathematical Sciences Clemson University October 6, 203 Outline
More informationSTABILITY. Phase portraits and local stability
MAS271 Methods for differential equations Dr. R. Jain STABILITY Phase portraits and local stability We are interested in system of ordinary differential equations of the form ẋ = f(x, y), ẏ = g(x, y),
More informationMath 20D: Form B Final Exam Dec.11 (3:00pm-5:50pm), Show all of your work. No credit will be given for unsupported answers.
Turn off and put away your cell phone. No electronic devices during the exam. No books or other assistance during the exam. Show all of your work. No credit will be given for unsupported answers. Write
More informationLinear Systems of ODE: Nullclines, Eigenvector lines and trajectories
Linear Systems of ODE: Nullclines, Eigenvector lines and trajectories James K. Peterson Department of Biological Sciences and Department of Mathematical Sciences Clemson University October 6, 2013 Outline
More informationNonlinear dynamics & chaos BECS
Nonlinear dynamics & chaos BECS-114.7151 Phase portraits Focus: nonlinear systems in two dimensions General form of a vector field on the phase plane: Vector notation: Phase portraits Solution x(t) describes
More informationLesson 4: Non-fading Memory Nonlinearities
Lesson 4: Non-fading Memory Nonlinearities Nonlinear Signal Processing SS 2017 Christian Knoll Signal Processing and Speech Communication Laboratory Graz University of Technology June 22, 2017 NLSP SS
More informationVideo 8.1 Vijay Kumar. Property of University of Pennsylvania, Vijay Kumar
Video 8.1 Vijay Kumar 1 Definitions State State equations Equilibrium 2 Stability Stable Unstable Neutrally (Critically) Stable 3 Stability Translate the origin to x e x(t) =0 is stable (Lyapunov stable)
More informationPerturbation Theory 1
Perturbation Theory 1 1 Expansion of Complete System Let s take a look of an expansion for the function in terms of the complete system : (1) In general, this expansion is possible for any complete set.
More informationClassification of Phase Portraits at Equilibria for u (t) = f( u(t))
Classification of Phase Portraits at Equilibria for u t = f ut Transfer of Local Linearized Phase Portrait Transfer of Local Linearized Stability How to Classify Linear Equilibria Justification of the
More information0 as an eigenvalue. degenerate
Math 1 Topics since the third exam Chapter 9: Non-linear Sstems of equations x1: Tpical Phase Portraits The structure of the solutions to a linear, constant coefficient, sstem of differential equations
More informationCopyright (c) 2006 Warren Weckesser
2.2. PLANAR LINEAR SYSTEMS 3 2.2. Planar Linear Systems We consider the linear system of two first order differential equations or equivalently, = ax + by (2.7) dy = cx + dy [ d x x = A x, where x =, and
More information= F ( x; µ) (1) where x is a 2-dimensional vector, µ is a parameter, and F :
1 Bifurcations Richard Bertram Department of Mathematics and Programs in Neuroscience and Molecular Biophysics Florida State University Tallahassee, Florida 32306 A bifurcation is a qualitative change
More informationContents lecture 6 2(17) Automatic Control III. Summary of lecture 5 (I/III) 3(17) Summary of lecture 5 (II/III) 4(17) H 2, H synthesis pros and cons:
Contents lecture 6 (7) Automatic Control III Lecture 6 Linearization and phase portraits. Summary of lecture 5 Thomas Schön Division of Systems and Control Department of Information Technology Uppsala
More informationMath 5490 November 12, 2014
Math 5490 November 12, 2014 Topics in Applied Mathematics: Introduction to the Mathematics of Climate Mondays and Wednesdays 2:30 3:45 http://www.math.umn.edu/~mcgehee/teaching/math5490-2014-2fall/ Streaming
More informationProblem Score Possible Points Total 150
Math 250 Fall 2010 Final Exam NAME: ID No: SECTION: This exam contains 17 problems on 13 pages (including this title page) for a total of 150 points. There are 10 multiple-choice problems and 7 partial
More informationStability lectures. Stability of Linear Systems. Stability of Linear Systems. Stability of Continuous Systems. EECE 571M/491M, Spring 2008 Lecture 5
EECE 571M/491M, Spring 2008 Lecture 5 Stability of Continuous Systems http://courses.ece.ubc.ca/491m moishi@ece.ubc.ca Dr. Meeko Oishi Electrical and Computer Engineering University of British Columbia,
More informationAPPPHYS217 Tuesday 25 May 2010
APPPHYS7 Tuesday 5 May Our aim today is to take a brief tour of some topics in nonlinear dynamics. Some good references include: [Perko] Lawrence Perko Differential Equations and Dynamical Systems (Springer-Verlag
More informationMATH 251 Examination II November 5, 2018 FORM A. Name: Student Number: Section:
MATH 251 Examination II November 5, 2018 FORM A Name: Student Number: Section: This exam has 14 questions for a total of 100 points. In order to obtain full credit for partial credit problems, all work
More informationLocal Phase Portrait of Nonlinear Systems Near Equilibria
Local Phase Portrait of Nonlinear Sstems Near Equilibria [1] Consider 1 = 6 1 1 3 1, = 3 1. ( ) (a) Find all equilibrium solutions of the sstem ( ). (b) For each equilibrium point, give the linear approimating
More informationMath 216 Second Midterm 28 March, 2013
Math 26 Second Midterm 28 March, 23 This sample exam is provided to serve as one component of your studying for this exam in this course. Please note that it is not guaranteed to cover the material that
More informationAppendix: A Computer-Generated Portrait Gallery
Appendi: A Computer-Generated Portrait Galler There are a number of public-domain computer programs which produce phase portraits for 2 2 autonomous sstems. One has the option of displaing the trajectories
More informationMAT 22B - Lecture Notes
MAT 22B - Lecture Notes 4 September 205 Solving Systems of ODE Last time we talked a bit about how systems of ODE arise and why they are nice for visualization. Now we'll talk about the basics of how to
More informationEven-Numbered Homework Solutions
-6 Even-Numbered Homework Solutions Suppose that the matric B has λ = + 5i as an eigenvalue with eigenvector Y 0 = solution to dy = BY Using Euler s formula, we can write the complex-valued solution Y
More informationNonlinear Autonomous Systems of Differential
Chapter 4 Nonlinear Autonomous Systems of Differential Equations 4.0 The Phase Plane: Linear Systems 4.0.1 Introduction Consider a system of the form x = A(x), (4.0.1) where A is independent of t. Such
More informationFundamentals of Dynamical Systems / Discrete-Time Models. Dr. Dylan McNamara people.uncw.edu/ mcnamarad
Fundamentals of Dynamical Systems / Discrete-Time Models Dr. Dylan McNamara people.uncw.edu/ mcnamarad Dynamical systems theory Considers how systems autonomously change along time Ranges from Newtonian
More informationAteneo de Manila, Philippines
Ideal Flow Based on Random Walk on Directed Graph Ateneo de Manila, Philippines Background Problem: how the traffic flow in a network should ideally be distributed? Current technique: use Wardrop s Principle:
More informationLocal Stability Analysis of a Mathematical Model of the Interaction of Two Populations of Differential Equations (Host-Parasitoid)
Biology Medicine & Natural Product Chemistry ISSN: 089-6514 Volume 5 Number 1 016 Pages: 9-14 DOI: 10.1441/biomedich.016.51.9-14 Local Stability Analysis of a Mathematical Model of the Interaction of Two
More informationSolutions Chapter 9. u. (c) u(t) = 1 e t + c 2 e 3 t! c 1 e t 3c 2 e 3 t. (v) (a) u(t) = c 1 e t cos 3t + c 2 e t sin 3t. (b) du
Solutions hapter 9 dode 9 asic Solution Techniques 9 hoose one or more of the following differential equations, and then: (a) Solve the equation directly (b) Write down its phase plane equivalent, and
More informationMath 304 Answers to Selected Problems
Math Answers to Selected Problems Section 6.. Find the general solution to each of the following systems. a y y + y y y + y e y y y y y + y f y y + y y y + 6y y y + y Answer: a This is a system of the
More informationEE16B Designing Information Devices and Systems II
EE6B M. Lustig, EECS UC Berkeley EE6B Designing Information Devices and Systems II Lecture 6B Cont. stability of Linear State Models Controllability Today Last time: Derived stability conditions for disc.
More informationSystems of Ordinary Differential Equations
Systems of Ordinary Differential Equations Scott A. McKinley October 22, 2013 In these notes, which replace the material in your textbook, we will learn a modern view of analyzing systems of differential
More informationDynamical Systems and Chaos Part I: Theoretical Techniques. Lecture 4: Discrete systems + Chaos. Ilya Potapov Mathematics Department, TUT Room TD325
Dynamical Systems and Chaos Part I: Theoretical Techniques Lecture 4: Discrete systems + Chaos Ilya Potapov Mathematics Department, TUT Room TD325 Discrete maps x n+1 = f(x n ) Discrete time steps. x 0
More informationMathematics Department, UIN Maulana Malik Ibrahim Malang, Malang, Indonesian;
P r o c e e d i n g I n t e r n a t i o n a l C o n f e r e n c e, 0 3, *, * * - * * The 4 th Green Technology Faculty of Science and Technology Islamic of University State Maulana Malik Ibrahim Malang
More informationMathematical Systems Theory: Advanced Course Exercise Session 5. 1 Accessibility of a nonlinear system
Mathematical Systems Theory: dvanced Course Exercise Session 5 1 ccessibility of a nonlinear system Consider an affine nonlinear control system: [ ẋ = f(x)+g(x)u, x() = x, G(x) = g 1 (x) g m (x) ], where
More informationNAME: MA Sample Final Exam. Record all your answers on the answer sheet provided. The answer sheet is the only thing that will be graded.
NAME: MA 300 Sample Final Exam PUID: INSTRUCTIONS There are 5 problems on 4 pages. Record all your answers on the answer sheet provided. The answer sheet is the only thing that will be graded. No books
More informationDynamics and Bifurcations in Predator-Prey Models with Refuge, Dispersal and Threshold Harvesting
Dynamics and Bifurcations in Predator-Prey Models with Refuge, Dispersal and Threshold Harvesting August 2012 Overview Last Model ẋ = αx(1 x) a(1 m)xy 1+c(1 m)x H(x) ẏ = dy + b(1 m)xy 1+c(1 m)x (1) where
More informationSection 5.5. Complex Eigenvalues
Section 5.5 Complex Eigenvalues Motivation: Describe rotations Among transformations, rotations are very simple to describe geometrically. Where are the eigenvectors? A no nonzero vector x is collinear
More informationPart II Problems and Solutions
Problem 1: [Complex and repeated eigenvalues] (a) The population of long-tailed weasels and meadow voles on Nantucket Island has been studied by biologists They measure the populations relative to a baseline,
More informationODE, part 2. Dynamical systems, differential equations
ODE, part 2 Anna-Karin Tornberg Mathematical Models, Analysis and Simulation Fall semester, 2011 Dynamical systems, differential equations Consider a system of n first order equations du dt = f(u, t),
More informationLab 5: Nonlinear Systems
Lab 5: Nonlinear Systems Goals In this lab you will use the pplane6 program to study two nonlinear systems by direct numerical simulation. The first model, from population biology, displays interesting
More informationMath 216 Final Exam 24 April, 2017
Math 216 Final Exam 24 April, 2017 This sample exam is provided to serve as one component of your studying for this exam in this course. Please note that it is not guaranteed to cover the material that
More informationProcedure for sketching bode plots (mentioned on Oct 5 th notes, Pg. 20)
Procedure for sketching bode plots (mentioned on Oct 5 th notes, Pg. 20) 1. Rewrite the transfer function in proper p form. 2. Separate the transfer function into its constituent parts. 3. Draw the Bode
More information6.2 Brief review of fundamental concepts about chaotic systems
6.2 Brief review of fundamental concepts about chaotic systems Lorenz (1963) introduced a 3-variable model that is a prototypical example of chaos theory. These equations were derived as a simplification
More informationCHALMERS, GÖTEBORGS UNIVERSITET. EXAM for DYNAMICAL SYSTEMS. COURSE CODES: TIF 155, FIM770GU, PhD
CHALMERS, GÖTEBORGS UNIVERSITET EXAM for DYNAMICAL SYSTEMS COURSE CODES: TIF 155, FIM770GU, PhD Time: Place: Teachers: Allowed material: Not allowed: January 08, 2018, at 08 30 12 30 Johanneberg Kristian
More informationHello everyone, Best, Josh
Hello everyone, As promised, the chart mentioned in class about what kind of critical points you get with different types of eigenvalues are included on the following pages (The pages are an ecerpt from
More informationMATH 251 Examination II April 4, 2016 FORM A. Name: Student Number: Section:
MATH 251 Examination II April 4, 2016 FORM A Name: Student Number: Section: This exam has 12 questions for a total of 100 points. In order to obtain full credit for partial credit problems, all work must
More informationMCE693/793: Analysis and Control of Nonlinear Systems
MCE693/793: Analysis and Control of Nonlinear Systems Systems of Differential Equations Phase Plane Analysis Hanz Richter Mechanical Engineering Department Cleveland State University Systems of Nonlinear
More information