On the convergence of solutions of the non-linear differential equation

Similar documents
(Received March 30, 1953)

On the stability of solutions of a system of differential equations

Maxima and Minima. (a, b) of R if

Engg. Math. I. Unit-I. Differential Calculus

Existence and uniqueness: Picard s theorem

1 The Existence and Uniqueness Theorem for First-Order Differential Equations

Nonlinear Control Systems

Lecture Notes in Functional Analysis

21-256: Partial differentiation

x 3y 2z = 6 1.2) 2x 4y 3z = 8 3x + 6y + 8z = 5 x + 3y 2z + 5t = 4 1.5) 2x + 8y z + 9t = 9 3x + 5y 12z + 17t = 7

Numerical Solution of Fuzzy Differential Equations

Nonlinear Systems and Control Lecture # 12 Converse Lyapunov Functions & Time Varying Systems. p. 1/1

A L A BA M A L A W R E V IE W

Math 131 Exam 2 Spring 2016

First order wave equations. Transport equation is conservation law with J = cu, u t + cu x = 0, < x <.

Math for Economics 1 New York University FINAL EXAM, Fall 2013 VERSION A

Lecture Notes on PDEs

First Order Differential Equations Lecture 3

Econ Lecture 14. Outline

Real Analysis, 2nd Edition, G.B.Folland Elements of Functional Analysis

Exercises for Multivariable Differential Calculus XM521

1 + x 2 d dx (sec 1 x) =

Introduction to Algebraic and Geometric Topology Week 3

Ordinary Differential Equations

Form A. 1. Which of the following is a second-order, linear, homogenous differential equation? 2

Analysis Comprehensive Exam Questions Fall F(x) = 1 x. f(t)dt. t 1 2. tf 2 (t)dt. and g(t, x) = 2 t. 2 t

("-1/' .. f/ L) I LOCAL BOUNDEDNESS OF NONLINEAR, MONOTONE OPERA TORS. R. T. Rockafellar. MICHIGAN MATHEMATICAL vol. 16 (1969) pp.

Math 4263 Homework Set 1

I. The space C(K) Let K be a compact metric space, with metric d K. Let B(K) be the space of real valued bounded functions on K with the sup-norm

Polytechnic Institute of NYU MA 2132 Final Practice Answers Fall 2012

ON THE AVERAGE NUMBER OF REAL ROOTS OF A RANDOM ALGEBRAIC EQUATION

Indian Institute of Technology Bombay

On a theorem of Weitzenbiick in invariant theory

The goal of this chapter is to study linear systems of ordinary differential equations: dt,..., dx ) T

ODE Homework 1. Due Wed. 19 August 2009; At the beginning of the class

Practice Problems for Exam 3 (Solutions) 1. Let F(x, y) = xyi+(y 3x)j, and let C be the curve r(t) = ti+(3t t 2 )j for 0 t 2. Compute F dr.

Find the slope of the curve at the given point P and an equation of the tangent line at P. 1) y = x2 + 11x - 15, P(1, -3)

2 Statement of the problem and assumptions

This property turns out to be a general property of eigenvectors of a symmetric A that correspond to distinct eigenvalues as we shall see later.

Linear DifferentiaL Equation

Chapter 1. Optimality Conditions: Unconstrained Optimization. 1.1 Differentiable Problems

Econ 204 Differential Equations. 1 Existence and Uniqueness of Solutions

PUTNAM PROBLEMS DIFFERENTIAL EQUATIONS. First Order Equations. p(x)dx)) = q(x) exp(

6.1 Matrices. Definition: A Matrix A is a rectangular array of the form. A 11 A 12 A 1n A 21. A 2n. A m1 A m2 A mn A 22.

Converse Lyapunov theorem and Input-to-State Stability

C o r p o r a t e l i f e i n A n c i e n t I n d i a e x p r e s s e d i t s e l f

Lecture two. January 17, 2019

Ordinary Differential Equation Theory

Old Math 330 Exams. David M. McClendon. Department of Mathematics Ferris State University

Solved Examples. Given are two sets A {1, 2, -2, 3} and B = {1, 2, 3, 5}. Is the function f(x) = 2x - 1 defined from A to B?

ANALYTIC TRANSFORMATIONS OF EVERYWHERE DENSE POINT SETS*

Examples include: (a) the Lorenz system for climate and weather modeling (b) the Hodgkin-Huxley system for neuron modeling

dx n a 1(x) dy

z x = f x (x, y, a, b), z y = f y (x, y, a, b). F(x, y, z, z x, z y ) = 0. This is a PDE for the unknown function of two independent variables.

I ƒii - [ Jj ƒ(*) \'dzj'.

Math 234. What you should know on day one. August 28, You should be able to use general principles like. x = cos t, y = sin t, 0 t π.

APPLICATIONS OF FD APPROXIMATIONS FOR SOLVING ORDINARY DIFFERENTIAL EQUATIONS

ON AN INFINITE SET OF NON-LINEAR DIFFERENTIAL EQUATIONS By J. B. McLEOD (Oxford)

Solutions to Final Exam Sample Problems, Math 246, Spring 2018

Real Analysis Math 131AH Rudin, Chapter #1. Dominique Abdi

Stability of Stochastic Differential Equations

Review For the Final: Problem 1 Find the general solutions of the following DEs. a) x 2 y xy y 2 = 0 solution: = 0 : homogeneous equation.

1 Definition and Basic Properties of Compa Operator

Entrance Exam, Differential Equations April, (Solve exactly 6 out of the 8 problems) y + 2y + y cos(x 2 y) = 0, y(0) = 2, y (0) = 4.

OH BOY! Story. N a r r a t iv e a n d o bj e c t s th ea t e r Fo r a l l a g e s, fr o m th e a ge of 9

Measure and Integration: Solutions of CW2

Problem Set 1. This week. Please read all of Chapter 1 in the Strauss text.

22.2. Applications of Eigenvalues and Eigenvectors. Introduction. Prerequisites. Learning Outcomes

UNIVERSITY OF MANITOBA

Call for Applications

2tdt 1 y = t2 + C y = which implies C = 1 and the solution is y = 1

Honours Analysis III

DRAFT - Math 101 Lecture Note - Dr. Said Algarni

F(p) y + 3y + 2y = δ(t a) y(0) = 0 and y (0) = 0.

Partial Differential Equations

Stochastic Differential Equations

ẋ = f(x, y), ẏ = g(x, y), (x, y) D, can only have periodic solutions if (f,g) changes sign in D or if (f,g)=0in D.

Economics 204 Fall 2011 Problem Set 2 Suggested Solutions

Math 205b Homework 2 Solutions

1+t 2 (l) y = 2xy 3 (m) x = 2tx + 1 (n) x = 2tx + t (o) y = 1 + y (p) y = ty (q) y =

Sample Questions Exam II, FS2009 Paulette Saab Calculators are neither needed nor allowed.

NOTE ON VOLTERRA AND FREDHOLM PRODUCTS OF SYMMETRIC KERNELS*

Topological properties

A Note on the Positive Nonoscillatory Solutions of the Difference Equation

u(0) = u 0, u(1) = u 1. To prove what we want we introduce a new function, where c = sup x [0,1] a(x) and ɛ 0:

LB 220 Homework 4 Solutions

EKOLOGIE EN SYSTEMATIEK. T h is p a p e r n o t to be c i t e d w ith o u t p r i o r r e f e r e n c e to th e a u th o r. PRIMARY PRODUCTIVITY.

Existence of the free boundary in a diffusive ow in porous media

1 h 9 e $ s i n t h e o r y, a p p l i c a t i a n

Functional Analysis. Martin Brokate. 1 Normed Spaces 2. 2 Hilbert Spaces The Principle of Uniform Boundedness 32

Problem Score Possible Points Total 150

Overview of normed linear spaces

CALCULUS MATH*2080 SAMPLE FINAL EXAM

Implicit Functions, Curves and Surfaces

3. Identify and find the general solution of each of the following first order differential equations.

Dr. Allen Back. Oct. 6, 2014

DEPARTMENT OF MATHEMATICS AND STATISTICS UNIVERSITY OF MASSACHUSETTS. MATH 233 SOME SOLUTIONS TO EXAM 2 Fall 2018

MATH 32A: MIDTERM 2 REVIEW. sin 2 u du z(t) = sin 2 t + cos 2 2

Diff. Eq. App.( ) Midterm 1 Solutions

Math Ordinary Differential Equations

Transcription:

MEMOIRS O F T H E COLLEGE O F SCIENCE, UNIVERSITY OF KYOTO, SERIES A Vol. XXVIII, Mathematics No. 2, 1953. On the convergence of solutions of the non-linear differential equation By Taro YOSHIZAWA (Received October 14, 1953) In the foregoing papar* we have researched sufficient conditions for the ultimate boundedness of solutions of the system of differential equations, (1) dx dt dy ' dt x, y) and we have obtained an existence theorem of a periodic solution by aid of the boundedness theorem. Namely under some conditions, it is proved that there exist two positive numbers A and B independent o f particular solutions such that lx(t)i ly(t)1<b for t t o (t o depending upon each particular solution), where WO, y (t)) is any solution of (1). Let f(t, x, y ) and g(t, x, y) be two continuous functions of (t, x, y) in the domain J,: --op <x<-1-00, 03 Ky<-1-00. Now we will show that under some conditions every solution of ( 1 ) converges to the periodic solution as t, c o provided the solutions of (1 ) are ultimately bounded. A t first, we shall prove two following lemmas. Lemma 1. L et j, be the 5-dimensional domain of (t, x, u, y, y) such as t o t <co, where t o m ay be arbitrarily great, but it is a constant. Now suppose * These Memoirs, Series A, Mathematics, Vol. 28, pp. 133-141.

144 T aro Yoshizawa that there ex ists a continuous function 0(x, u, y, v ) satisfying the following conditions in J2 ; namely 10 0(x, u, y, v)> 0, provided Ix ui +ly vj> 0, 200(x, u, y, v) =0, prov ided Ix + ly v1.-- 0, 3 0 0 (x, u, y, v) satisfies the Lipschitz condition w ith regard to (x, u, y, v ) and for every point in the interior of this dom ain J we have 1 urn {0(x+hf(t, x,y), u+hf(t, u, v), y+hg(t, x,y), v+hg(t, v ) ) h40 h (x, u, y, where for every A> 0 (small alone being w orth to consider), if Ix + ly vl the lef t hand side o f this inequality x(2) <0 (x(2) m ay be arbitrarily sm all, but it is a fixed constant for fixed A). Then choosing 4(> 0) suitably f o r any e> 0 (e however small), if any two solutions of (1), (x(t), y(t)) and ( X(t), 5)(t)), which satisfy xi <A, lyi <B for satisfy the following inequality at t---t ( T being arbitrary), (2)!x(T) :x(t) 1+ ly(t) :y(t) <a, then f o r t> T we have always (3) x(t) (t) + ly(0-s, (01 <. P roof. For a given g, let 4' be the minimum of 0(x, u, y, v) when lx ul + ly-v1-=e. Then since 0(x, u, y, y ) is positive for Ix u I + ly vi > 0, it is clear that a'> 0, and 4' is independent of t. Moreover since 0(x, u, y, v) satisfies the Lipschitz condition, we have a positive constant K such as I 0(x, u, y, y) GO(x', u', y', /01-<K(1/ x'i Now we put a=m in (47K, e). + I + IY-Y1+1Y-v'1). Then it is proved as follows that for any two solutions (x(t), y(t)) and (i(t), j)(t)) satisfying (2) at an arbitrary t T, the inequality (3 ) holds good : Namely i f otherwise suppose that we have at some t = r

O n the convergence of solutions of the non-linear. 145 lx (r) - - i(r)1 + 1 Y (T ) - - (T')I = E Now consider th e function (P(x(t), y(t), :9(t)) for T t _ T ' and then 0.;_a' at t=t ', while we have (4) 0(x(T), y(t), since this function is a non-increasing function of t by the condition 3 0. Moreover we have Go(x(T), 3:(T), y (T), 51(T)) ( - Hence we have (T),.i(T), 5,(T), ji(t)) < K (Ix (T )--i(t ) -1-1Y (T )-5 1 (T)l) Ka < K a' /K =6'. for by the condition 2 0(x(T), Ti(T), y(t), 5,(T)) <4', 0 (i(7 ), Tx(T), :9(T), :9(T))=0. This contradicts (4) and hence (3) holds good. Thus the proof is completed. Lemma 2. S uppose that the sam e assum ptions a s those in Lemma 1 hold good. T hen giv en any positiv e num ber ô (a may be sufficiently small), it for any two solutions of (1) (x(t), y(t)) and W O, jr(t)) which satisfy ix i <A, lyi <B f o r t>_t w e have at some t T (>_t o ) ( T being arbitrary, but fixed) (5) Ix(T)--(T)1+1,y(T)--.9(T)1.> 4, then ive have at som e T ' (> and (6) IA(T')-- 7")I+IY(r)--5/(T')I < 4. P ro o f. Let J., and 4 1 be two dom ains such as T<t<00, lx ul+ly vi <4' IvK B respectively, where a' <..a. Now consider a function (t, x, u, y, e t (x, u, y, v) (N> 0) in 4 3. j4 and then we have

146 Taro Yoshizawa. 1 (t, x, u, y, v)> 0, since I x vl> 0, 2 V (t, x, u, y, v) tends to infinity uniformly for (x, u, y, y) as C O. And it is c le a r th a t T(t, x, u, y, v ) satisfies locally for t the Lipschitz condition w ith regard to (x, u, y, y). Moreover we have lirn h.4.0 l {hr(t+h,x+hf(t,x,y ),u+hf(t,u,v),y+hg(t,x,y), h v + hg(t, u, v)) (t, x, u, y, v)} =11m 1 i e " - fh) (x+ hf, u+ hf, y+ hg, v+ hg) e'0 (x, u, y, v)} h 4 0 h =lim 1 le N" - "10 (x+ hf, u + hf, y + hg, v+ hg) (x, u, y, v)] n - O h + (en"+h ) e")0 (x, u, y, v)} =e' lim 1 [ 0(x+ hf, u + hf, y+ hg, v+ hg) 0(x, u, y, v,)] h +N (I) (I, u, y, v) e`" ((Y ) +NO (x, u, y, 01-. Now for 3', w e can choose N (6') so sm a ll th a t th is expression become a lw a y s non-positive in the interior of 43-4 4. Therefore 3 r(t, x, u, y, v) satisfies locally the Lipschitz condition w ith regard to (x, u, y, y) and for a ll points in the interior of J., J,, w e have lim it(t+ h, x+ hf(t, y), u+ hf(t, u, v), y+ hg(t, x, y). h v+ hg(t, u, u, y, v)} Now suppose that the assertion (6) is not true for 3. Let 4, and J be two domains such as and Ix + vl <4

O n the convergence of solutions of the non-linear. 147 respectively. Then we can choose T " by 2 0 such that (7) min ev ' "(.b(x, u, y, y) > max e - ( 6 ) V ( 8 1 ) T (X, u, y, v), A 5 -A 8 As Aa while by 3 (T ", x(t "),i(t ''), y(t "), -51(T"))_er (T, x(t),i(t), y(t),s)(t)). This contradicts (7 ). Therefore the assertilin is tru e. T h is T" depends upon T and N (ô'). Now we can prove the following convergence theorem by aid of these lemmas. Theorem 1. Suppose that the solutions of (1) are ultimately bounded f o r A an d B and that the sam e assum ptions a s those in Lemma 1 hold good. Then f o r any two solutions o f (1) (x(t), y ( t) an d (i (t), A t)), w e have (x (t)- ī(t))= 0 (8) lim (y (t)-5)(t)) =O. P ro o f Let (x(t), y ( 0 ) and (t), Ȳ (t)) be any two solutions of (1 ). Then since these are ultimately bounded with the bounds A and B, there exist T, and T, such that and Ix(t) I <A, ly(t) 1 <B for ii(01 <A, I -51(01 <B for t- T2 respectively. Now we put T= max (T T t0 ). By Lemma 1, a is chosen for an e> 0 (however small) and if, for this a, we do not have then we can choose T such as ix (T) + ( T ) <d, Ix(T) i(r) I + Y (T) 5)(T)1 <a by Lemma 2, where T ' -> T. Then by Lemma 1 we have lx(t) - - i(t) + Iy (t) 5)(t) < E, for t> T '. Namely (8) holds good. From this fact, it is easy to prove the following theorem. Theorem 2. If the sam e assum ptions a s those in Theorem 1

148 T aro Yoshizawa hold good and the system of dwerential equations (1) has a periodic solution of period i t i s unique and the other solutions of (1) converge to that periodic solution as t co. Rem ark. If 0(x, u, y, v) in condition 3 be totally differentiable, then the inequality under 3 reduces to a (x, u, y, v)./. (t, y ) a o ( x, u, y, v) f ( t, u, v ) ax au 30 (x, u, y, v) a(1)(x u v) g(t, x, y) + ' " y g ( t, u, v ) _ <0. av Instead o f sufficient conditions under w hich the results of Theorems 1 and 2 are concluded, we can modify the conditions in Lemma 1 and those in Lemma 2 independently as follows. Namely Lemma 3. Suppose that there exists a continuous function of x, u, y, v) (1)(t, x, u, y, v ) in 4, satisfying the following conditions ; namely 1 (t, x, u, y, v) = 0, provided Ix y v1=0, 2 there exists a positive num ber d(e) such that (t, x, u, y, v) > a(e)> 0 when Ix tti +ly vi s, where e is an arbitrary positive num ber and 1 depends on E, 3 0(4 x, u, y, v) satisfies the Lipschitz condition with regard to (x, u, y, v) and f o r a positive constant K, and in the interior of 4 2 w e have. 1 -- ( t + h, x+ hf(t, x, y ), u+ hf(t, u, v), y+ hg(t, x, y), h v+ hg(t, u, v)) (t, x, u, y, v)} Then f o r any tw o solutions of (1 ), (x (t),y (t)) and (i(t),y (t)) satisfying ix l < A, I <B J r t t, being given a n arbitrary positive num ber e (however small), there exists a positive num ber 2( <e) independent of T such that, i f w e hav e for an arbitrary T (_t ) then (9) lx(t)--i(t)i +1), (7') (10) lx(t) i(t) + 1.Y(1) - - (t)1 holds for t>_t. Rem ark. Since the case where e is small alone is worth to

O n the convergence of solutions of the non-linear. 149 consider, it is sufficient that the condition 3 is satisfied in the domain in 4 2 such as to t<co, where x(> 0 ) may be sufficiently small. Of course it is sufficient that 0 exists in the domain where Ix ui + ly v1 is sufficiently small. P roof. For an e, choosing A such as 4E) <min (ax, e), this À depends only on e. Now suppose that, for any two solutions of (1 ) now considering (x (t), y (t)) and W O, 5)(t) ) satisfying (9) at t T, we have at some t(> T ), say T', (11) lx (T ')--i(t ') I+ Y (T ') ( 7 ")1=e. Then we can consider this T ' as the first t where (11) holds by the continuity of the solutions. Hence by considering the function (t, x (t), (t), y (t), Si (t)) for, the conclusion of this lemma follows in the same way as in Lemma 1. This first T ' is taken according to the fact mentioned in the above remark. Lemma 4. For every a->o (a may be sufficiently small), let 4 7 be the dom ain such as t o _ t<co, lx ul + ly vl <a. S uppose that there ex ists a continuous function of (t, x, u, y v), qr,(t, x, u, y, v) (t, x, u, y, v ), in 4 2 47 which satisfies the following conditions ; namely 1 qr (t, x, u, y, v ) is positive in 42 4 7, 2 (t, x, u, y, v) tends to zero uniformly for (x, u, y, v) when t co (or tends to infinity uniformly a s t. co), 3 F (t, x, u, y, v) satisfies locally the Lipschitz condition with regard to (x, u, y, v) and in th e interior o f this domain 4 7, w e have. 1 {IT (t + h, x+ x, y), u + hf(t, u, v), y + hg(t, x, y), h + 0 h v+ hg(t, u, v)) (t, x, u, y, v)}

150 T aro Yoshizawa (or lim 1 If (t+h,x+hf,u+lif,y+hg,v+hg) h+0 h (t, x, u, y, v)} Then f o r any two solutions of (1 ) (x (t),y (t)) an d (i(t), (t)) satisfying lxi < A,Iy I< B f o r t_t, if w e have at some t T(>_t o) lx(t) i(t)1+1y(t)-51(t)i> a, then at some T ' such as r> T, we have lx(t')--4(t')1+iy(t')---51(p)i a. The proof is omitted, for it is the same with Lemma 2. Theorem 3. If the solutions of (1) are ultimately bounded for A and B and the assumptions in Lemmas 3 and 4 hold good, then we have (8) f o r any tw o solutions of (1 ), (x (t),y (t)) an d W O, 3i (t)). Rem ark. Theorems 1, 2 a n d 3 can be generalized for the m ore general system o f differential equations dx, ( i f J s \. ) dt 1. 1, X 21, x ) (1-1, 2 n). Exam ple. Reuter has obtained a convergence theorem for the solutions of the differential equation of the second order (12) i+ kf(x)i+g(x) kp(t) (k> 0) in the Journal of the L ondon Mathematical Society, Vol. 26 (1951). Together w ith conditions for the ultim ate boundedness, he has supposed that g' (x)> 0 and that g" (x) e x is ts and is bounded for Here x, corresponds to A in our theorem s. And using his notations, w e have lx(t)1 J o and * 0 1 Thus there exist positive constants a,, 6 4> a4 and 1- (x0), independent of k, such that fo r ix I <x o la,_< f(x) 5a 2 a g '(x )._.._a, Ig"(x)I_- )- (x0), by the assumptions for f(x ), g i(x ) and g ' (x ). A n d he concludes th a t, i f k>k --v or(x )/a,a th en fo r a n y tw o solutions of (12), (x, (t), :x, (t )) and (x2(t), i2 ( t) ), w e have

On the convergence of solutions o f the non-linear. 151 x2 (t).x,(t)--)0 and i2(t) (t) 0 as co. For our part, instead of (12), we consider the system (13) i= y kf(x), g(x)+kp(t), where F(x )=ff(x )dx. Then for 0(x, u, y, v) in Theorem 1, we may take the expression (14) (g(x) g(u))(x u)+(y v)'-2c(x u)(y v) which Reuter has denoted by Q and used it in his research, where c is a positive suitable constant and is chosen so sm all that (14) is positive definite with regard to (x u) and (y v).