Math 5490 November 5, 2014

Similar documents
Math 5490 November 12, 2014

Math 312 Lecture Notes Linearization

Def. (a, b) is a critical point of the autonomous system. 1 Proper node (stable or unstable) 2 Improper node (stable or unstable)

Nonlinear Autonomous Dynamical systems of two dimensions. Part A

Autonomous systems. Ordinary differential equations which do not contain the independent variable explicitly are said to be autonomous.

2.10 Saddles, Nodes, Foci and Centers

Phase Plane Analysis

Chapter 6 Nonlinear Systems and Phenomena. Friday, November 2, 12

Problem set 7 Math 207A, Fall 2011 Solutions

Lecture 38. Almost Linear Systems

Math 3301 Homework Set Points ( ) ( ) I ll leave it to you to verify that the eigenvalues and eigenvectors for this matrix are, ( ) ( ) ( ) ( )

Classification of Phase Portraits at Equilibria for u (t) = f( u(t))

Continuous Threshold Policy Harvesting in Predator-Prey Models

1 Introduction Definitons Markov... 2

Calculus and Differential Equations II

Nonlinear Dynamics of Neural Firing

Find the general solution of the system y = Ay, where

ODE, part 2. Dynamical systems, differential equations

MATH 614 Dynamical Systems and Chaos Lecture 24: Bifurcation theory in higher dimensions. The Hopf bifurcation.

MathQuest: Differential Equations

Math 331 Homework Assignment Chapter 7 Page 1 of 9

April 13, We now extend the structure of the horseshoe to more general kinds of invariant. x (v) λ n v.

3 Stability and Lyapunov Functions

Math 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

Di erential Equations

Physics: spring-mass system, planet motion, pendulum. Biology: ecology problem, neural conduction, epidemics

Math 266: Phase Plane Portrait

0 as an eigenvalue. degenerate

Chapter 9 Global Nonlinear Techniques

Math 215/255: Elementary Differential Equations I Harish N Dixit, Department of Mathematics, UBC

= F ( x; µ) (1) where x is a 2-dimensional vector, µ is a parameter, and F :

MATH 215/255 Solutions to Additional Practice Problems April dy dt

Section 5.4 (Systems of Linear Differential Equation); 9.5 Eigenvalues and Eigenvectors, cont d

Student name: Student ID: Math 265 (Butler) Midterm III, 10 November 2011

Hello everyone, Best, Josh

7 Planar systems of linear ODE

1. For each function, find all of its critical points and then classify each point as a local extremum or saddle point.

6.3. Nonlinear Systems of Equations

ENGI Linear Approximation (2) Page Linear Approximation to a System of Non-Linear ODEs (2)

Vectors, matrices, eigenvalues and eigenvectors

An Undergraduate s Guide to the Hartman-Grobman and Poincaré-Bendixon Theorems

Stability of Dynamical systems

8.1 Bifurcations of Equilibria

1 The pendulum equation

Problem set 6 Math 207A, Fall 2011 Solutions. 1. A two-dimensional gradient system has the form

Vector Field Topology. Ronald Peikert SciVis Vector Field Topology 8-1

Math 232, Final Test, 20 March 2007

MTH4101 CALCULUS II REVISION NOTES. 1. COMPLEX NUMBERS (Thomas Appendix 7 + lecture notes) ax 2 + bx + c = 0. x = b ± b 2 4ac 2a. i = 1.

Math 4B Notes. Written by Victoria Kala SH 6432u Office Hours: T 12:45 1:45pm Last updated 7/24/2016

PHY411 Lecture notes Part 5

MAT 22B - Lecture Notes

8 Vector Field Topology

Models Involving Interactions between Predator and Prey Populations

MATH 251 Final Examination December 16, 2015 FORM A. Name: Student Number: Section:

Some Dynamical Behaviors In Lorenz Model

DYNAMICAL SYSTEMS. I Clark: Robinson. Stability, Symbolic Dynamics, and Chaos. CRC Press Boca Raton Ann Arbor London Tokyo

Kinematics of fluid motion

Local Phase Portrait of Nonlinear Systems Near Equilibria

Math 53 Homework 7 Solutions

154 Chapter 9 Hints, Answers, and Solutions The particular trajectories are highlighted in the phase portraits below.

Math 216 First Midterm 19 October, 2017

Bifurcation Analysis of Non-linear Differential Equations

Solutions 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

Half of Final Exam Name: Practice Problems October 28, 2014

Characterization of the stability boundary of nonlinear autonomous dynamical systems in the presence of a saddle-node equilibrium point of type 0

Differential Equations 2280 Sample Midterm Exam 3 with Solutions Exam Date: 24 April 2015 at 12:50pm

Global Stability Analysis on a Predator-Prey Model with Omnivores

Part II Problems and Solutions

Announcements Wednesday, November 7

Fundamentals of Dynamical Systems / Discrete-Time Models. Dr. Dylan McNamara people.uncw.edu/ mcnamarad

ENGI Duffing s Equation Page 4.65

Bishop Kelley High School Summer Math Program Course: Honors Pre-Calculus

CHAPTER 6 HOPF-BIFURCATION IN A TWO DIMENSIONAL NONLINEAR DIFFERENTIAL EQUATION

1. (a) (5 points) Find the unit tangent and unit normal vectors T and N to the curve. r (t) = 3 cos t, 0, 3 sin t, r ( 3π

MATH 251 Final Examination December 19, 2012 FORM A. Name: Student Number: Section:

B5.6 Nonlinear Systems

Coupled differential equations

STABILITY. Phase portraits and local stability

Solutions to Test #1 MATH 2421

Dynamics and Bifurcations in Predator-Prey Models with Refuge, Dispersal and Threshold Harvesting

Section 4.5. Integration and Expectation

In these chapter 2A notes write vectors in boldface to reduce the ambiguity of the notation.

Note: Each problem is worth 14 points except numbers 5 and 6 which are 15 points. = 3 2

Nonlinear Autonomous Systems of Differential

ENGI Partial Differentiation Page y f x

Travelling waves. Chapter 8. 1 Introduction

Chapter 8 Equilibria in Nonlinear Systems

Department of Mathematics IIT Guwahati

Topic # /31 Feedback Control Systems. Analysis of Nonlinear Systems Lyapunov Stability Analysis

ANSWERS Final Exam Math 250b, Section 2 (Professor J. M. Cushing), 15 May 2008 PART 1

CHAPTER 5 KINEMATICS OF FLUID MOTION

Sample Solutions of Assignment 10 for MAT3270B

Math 216 Final Exam 24 April, 2017

Course Outline. 2. Vectors in V 3.

Pullbacks, Isometries & Conformal Maps

Outline. Learning Objectives. References. Lecture 2: Second-order Systems

Section 9.3 Phase Plane Portraits (for Planar Systems)

MATH 415, WEEK 11: Bifurcations in Multiple Dimensions, Hopf Bifurcation

Math 265 (Butler) Practice Midterm III B (Solutions)

Nonlinear dynamics & chaos BECS

Transcription:

Math 549 November 5, 214 Topics in Applied Mathematics: Introduction to the Mathematics of Climate Mondays and Wednesdays 2:3 3:45 http://www.math.umn.edu/~mcgehee/teaching/math549-214-2fall/ Streaming video is available at http://www.ima.umn.edu/videos/ Click on the link: "Live Streaming from 35 Lind Hall". Participation: https://umconnect.umn.edu/mathclimate

Classification trace determinant Kaper & Engler, 213

Topological Classification If neither eigenvalue has zero real part, then the system is called hyperbolic, in which case, there are only three classes: 1. saddles: One positive eigenvalue and one negative. The determinant is negative. 2. sources: Both eigenvalues have positive real part. The determinant is positive, and the trace is positive. 3. sinks: Both eigenvalues have negative real part. The determinant is positive, and the trace is negative. Every system in one of the three categories looks the same to a topologist (topological conjugacy).

Topological Classification saddle source trace sink determinant

Topological Classification Saddles : det < 2 1 1 saddle source trace/2 2 2 2 1 1 2 trace determinant 1 sink 1 determinant 2 2 1 1 2

Topological Classification Saddles : det < source saddle trace sink determinant

Topological Classification Sources det >, trace > 2 1 1 saddle source trace 2 2 2 1 1 2 trace determinant 1 sink 1 determinant 2 2 1 1 2

Topological Classification Sources det >, trace > source saddle trace sink determinant

Topological Classification Sinks det >, trace < 2 1 1 saddle source trace 2 2 2 1 1 2 trace determinant 1 sink 1 determinant 2 2 1 1 2

Topological Classification Sinks det >, trace < source saddle trace sink determinant

Topological Classification All sources look the same. Everything leaves.

Topological Classification All sinks look the same. Everything approaches the origin asymptotically.

Topological Classification One Variable x u u Let x u u u u u u 1 du u x u du u 1 Continuous, but not smooth at. u x du 1 du u u x 1 x u u du u

Topological Classification Two Variables Saddles dy x x 1 x u u 1 y v v du dv u v Continuous, but not smooth at (,). topologically conjugate

Topological Classification Sinks dy x x 1 x u u 1 y v v du dv u v Continuous, but not smooth at (,). topologically conjugate

Topological Classification What about spirals? dz ( 1 ) ix i ilog w z w we w Continuous, but not smooth at. dw w

Topological Classification Computation i dz i i 21 ( 1 iz ) ( ) i i 2 i 2 i 21 i 2 1 1 i 2 i 2 z w w ww w w w dz z w ww w w w 2 2 i Multiply by w w i i i 1 i w 2 w w w w 2 w complex conjugate i i (1 iz ) (1 i) w w 1 ww i ww (1 i) ww ww ww 2ww i i 1 ww ww 2 ww (1 i) ww 2 2 2 2 i i 2 2 ww 1 ww (1 i) ww ww ww 2ww ww iww (1 i) ww ww ww dw w add

Topological Classification What about spirals? dz ( 1 ) ix i ilog w z w we w Continuous, but not smooth at. dw w

Topological Classification All sinks are topologically conjugate, as are all sources and all saddles.

Topological Classification saddle source trace sink determinant

Rest points: Dynamical Systems Nonlinear Systems One Variable f ( x) f( x) If f( p), then x( t) p (constant) is a solution. Example x x 3 Rest points: 3 x x x 1 x 1 x 1,, and 1

Nonlinear Systems One Variable Rest points Example 2 x x 3 1 f(x) What about the stability of the rest points? 1 2 2 1 1 2 x

Nonlinear Systems One Variable Rest points Example 2 x x 3 1 f(x) What about the stability of the rest points? 1 2 2 1 1 2 x

Nonlinear Systems f ( x) Rest point p : f( p) Linear approximation: f ( x) f ( p) f ( p)( x p) f ( p)( x p) Introduce x p. Then f( x) f( p ) f( p) d f( x) f( p ) f( p) Basic Idea If is small, i.e., if x is close to p, d then solutions of f( p) d are close to solutions of f ( p). In particular, the rest point p is asymptotically stable for f ( x) d if the origin is asymptotically stable for f( p).

Nonlinear Systems f ( x) Rest point p : f( p) Criteria The rest point p is asymptotically stable for f( x) if f( p). It is unstable if f( p).

Nonlinear Systems Example f ( x) x x 3 2 stable Rest points: 1,, and 1 f( x) 13x f( 1) f(1) 2, f() 1 Rest points 1 and 1 are stable, rest point is unstable. 2 f(x) 1 1 2 2 1 1 2 x unstable

Nonlinear Systems Two Variables 1 f1( x1, x2) 2 f2( x1, x2) f( x), x, f : 2 2 2 f( x) If f( p), then x( t) p (constant) is a solution (rest point) f( p) f ( p, p ) 1 1 2 f ( p, p ) 1 1 2 x () t p 1 1 x () t p 1 1

Nonlinear Systems dy Example 3 x x y y Rest points: x x 3 y x x 3 x 1 x 1 x y y y ( 1,), (,), and (1,)

If y(), then y( t), for all t. invariant line : x axis Dynamical Systems Nonlinear Systems Example dy 3 x x y y y rest points x How do we analyze the full system?

Nonlinear Systems 3 x x y dy y Preview

Nonlinear Systems Jacobian Matrix 1 2 f ( x, x ) f 1 1 2 ( x, x ) 2 1 2 f( x), x, f : 2 2 2 Df ( x) f1 f1 ( x1, x2) ( x1, x2) x1 x 2 f2 f ( x 2 1, x2) ( x1, x2) x1 x 2

Nonlinear Systems Example dy 3 x x y y Df ( x, y) 2 1 3x 1 1 2 1 1 1 2 1 Df ( 1,) Df (,) Df (1,) 1 1 1

Nonlinear Systems f ( x) Rest point p : f( p) Linear approximation: f ( x) f ( p) Df ( p)( x p) Df ( p)( x p) Introduce x p. Then f( x) f( p ) Df( p) d f( x) f( p ) Df( p) Basic Idea If is small, i.e., if x is close to p, d then solutions of f( p) d are close to solutions of Df ( p). In particular, the rest point p is asymptotically stable for f ( x) d if the origin is asymptotically stable for Df ( p).

Nonlinear Systems f ( x) Rest point p : f( p) Criteria The rest point p is saddle for f( x) if det D f( p). It is a source if det D ( ) and trace D ( ). f p f p f p f p It is a source if det D ( ) and trace D ( ).

dy Dynamical Systems 3 x x y y Nonlinear Systems Example Rest points: ( 1,), (,), and (1,) 2 1 1 1 2 1 Df ( 1,) Df (,) Df (1,) 1 1 1 det D f ( 1,) 2 trace D f ( 1,) 3 sink 2 discriminant D f ( 1,) ( 3) 4 2 1 det D f (,) 1 saddle stable node

If y(), then y( t), for all t. invariant line : x axis Dynamical Systems Nonlinear Systems Example dy 3 x x y y y rest points x stable node saddle