ASYMPTOTIC FORMS OF WEAKLY INCREASING POSITIVE SOLUTIONS FOR QUASILINEAR ORDINARY DIFFERENTIAL EQUATIONS

Similar documents
Asymptotic instability of nonlinear differential equations

The Asymptotic Behavior of Nonoscillatory Solutions of Some Nonlinear Dynamic Equations on Time Scales

Ann. Funct. Anal. 2 (2011), no. 2, A nnals of F unctional A nalysis ISSN: (electronic) URL:

EXISTENCE OF NON-OSCILLATORY SOLUTIONS TO FIRST-ORDER NEUTRAL DIFFERENTIAL EQUATIONS

Properties Of Solutions To A Generalized Liénard Equation With Forcing Term

Hamilton- J acobi Equation: Weak S olution We continue the study of the Hamilton-Jacobi equation:

On a Fractional Stochastic Landau-Ginzburg Equation

Existence of positive solution for a third-order three-point BVP with sign-changing Green s function

Math 2142 Exam 1 Review Problems. x 2 + f (0) 3! for the 3rd Taylor polynomial at x = 0. To calculate the various quantities:

Oscillation of an Euler Cauchy Dynamic Equation S. Huff, G. Olumolode, N. Pennington, and A. Peterson

23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes

Challenge Problems. DIS 203 and 210. March 6, (e 2) k. k(k + 2). k=1. f(x) = k(k + 2) = 1 x k

A Necessary and Sufficient Condition for the Solutions of a Functional Differential Equation to Be Oscillatory or Tend to Zero

EXERCISES FOR SECTION 1.5

Existence Theory of Second Order Random Differential Equations

On Oscillation of a Generalized Logistic Equation with Several Delays

Chapter 2. First Order Scalar Equations

STABILITY OF NONLINEAR NEUTRAL DELAY DIFFERENTIAL EQUATIONS WITH VARIABLE DELAYS

CERTAIN CLASSES OF SOLUTIONS OF LAGERSTROM EQUATIONS

POSITIVE SOLUTIONS OF NEUTRAL DELAY DIFFERENTIAL EQUATION

An Introduction to Malliavin calculus and its applications

LIMIT AND INTEGRAL PROPERTIES OF PRINCIPAL SOLUTIONS FOR HALF-LINEAR DIFFERENTIAL EQUATIONS. 1. Introduction

Existence of positive solutions for second order m-point boundary value problems

Matrix Versions of Some Refinements of the Arithmetic-Geometric Mean Inequality

A Note on Superlinear Ambrosetti-Prodi Type Problem in a Ball

CHARACTERIZATION OF REARRANGEMENT INVARIANT SPACES WITH FIXED POINTS FOR THE HARDY LITTLEWOOD MAXIMAL OPERATOR

23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes

Final Spring 2007

Undetermined coefficients for local fractional differential equations

arxiv: v1 [math.ca] 15 Nov 2016

Representation of Stochastic Process by Means of Stochastic Integrals

arxiv:math/ v1 [math.nt] 3 Nov 2005

EXISTENCE AND UNIQUENESS THEOREMS ON CERTAIN DIFFERENCE-DIFFERENTIAL EQUATIONS

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle

Solutions to Assignment 1

Convergence of the Neumann series in higher norms

MATH 4330/5330, Fourier Analysis Section 6, Proof of Fourier s Theorem for Pointwise Convergence

Bernoulli numbers. Francesco Chiatti, Matteo Pintonello. December 5, 2016

2. Nonlinear Conservation Law Equations

arxiv: v1 [math.fa] 9 Dec 2018

TO our knowledge, most exciting results on the existence

t is a basis for the solution space to this system, then the matrix having these solutions as columns, t x 1 t, x 2 t,... x n t x 2 t...

BOUNDED VARIATION SOLUTIONS TO STURM-LIOUVILLE PROBLEMS

Stability and Bifurcation in a Neural Network Model with Two Delays

DIFFERENTIAL EQUATIONS

Physics 127b: Statistical Mechanics. Fokker-Planck Equation. Time Evolution

Robust estimation based on the first- and third-moment restrictions of the power transformation model

Monotonic Solutions of a Class of Quadratic Singular Integral Equations of Volterra type

Positive continuous solution of a quadratic integral equation of fractional orders

On Two Integrability Methods of Improper Integrals

Predator - Prey Model Trajectories and the nonlinear conservation law

Solutions from Chapter 9.1 and 9.2

Endpoint Strichartz estimates

SOLUTIONS APPROACHING POLYNOMIALS AT INFINITY TO NONLINEAR ORDINARY DIFFERENTIAL EQUATIONS

Some New Uniqueness Results of Solutions to Nonlinear Fractional Integro-Differential Equations

Simulation-Solving Dynamic Models ABE 5646 Week 2, Spring 2010

Linear Response Theory: The connection between QFT and experiments

4 Sequences of measurable functions

MATH 128A, SUMMER 2009, FINAL EXAM SOLUTION

OSCILLATION CONSTANT FOR MODIFIED EULER TYPE HALF-LINEAR EQUATIONS

MA 214 Calculus IV (Spring 2016) Section 2. Homework Assignment 1 Solutions

Existence of multiple positive periodic solutions for functional differential equations

WEIGHTED PSEUDO PERIODIC SOLUTIONS OF NEUTRAL FUNCTIONAL DIFFERENTIAL EQUATIONS

1 1 + x 2 dx. tan 1 (2) = ] ] x 3. Solution: Recall that the given integral is improper because. x 3. 1 x 3. dx = lim dx.

Differential Equations

BOUNDEDNESS OF MAXIMAL FUNCTIONS ON NON-DOUBLING MANIFOLDS WITH ENDS

Optimality Conditions for Unconstrained Problems

arxiv: v1 [math.gm] 4 Nov 2018

Boundedness and Exponential Asymptotic Stability in Dynamical Systems with Applications to Nonlinear Differential Equations with Unbounded Terms

Dynamic Systems and Applications 12 (2003) A SECOND-ORDER SELF-ADJOINT EQUATION ON A TIME SCALE

Existence of non-oscillatory solutions of a kind of first-order neutral differential equation

Echocardiography Project and Finite Fourier Series

On Carlsson type orthogonality and characterization of inner product spaces

R t. C t P t. + u t. C t = αp t + βr t + v t. + β + w t

THE SINE INTEGRAL. x dt t

A NOTE ON S(t) AND THE ZEROS OF THE RIEMANN ZETA-FUNCTION

This document was generated at 1:04 PM, 09/10/13 Copyright 2013 Richard T. Woodward. 4. End points and transversality conditions AGEC

dt = C exp (3 ln t 4 ). t 4 W = C exp ( ln(4 t) 3) = C(4 t) 3.

10. State Space Methods

dy dx = xey (a) y(0) = 2 (b) y(1) = 2.5 SOLUTION: See next page

The Contradiction within Equations of Motion with Constant Acceleration

CONTRIBUTION TO IMPULSIVE EQUATIONS

Section 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients

Oscillation of solutions to delay differential equations with positive and negative coefficients

KEY. Math 334 Midterm I Fall 2008 sections 001 and 003 Instructor: Scott Glasgow

Mapping Properties Of The General Integral Operator On The Classes R k (ρ, b) And V k (ρ, b)

The L p -Version of the Generalized Bohl Perron Principle for Vector Equations with Infinite Delay

EIGENVALUE PROBLEMS FOR SINGULAR MULTI-POINT DYNAMIC EQUATIONS ON TIME SCALES

KEY. Math 334 Midterm III Winter 2008 section 002 Instructor: Scott Glasgow

Ordinary Differential Equations

Chapter 7: Solving Trig Equations

Approximation Algorithms for Unique Games via Orthogonal Separators

Class Meeting # 10: Introduction to the Wave Equation

8. Basic RL and RC Circuits

Research Article Existence and Uniqueness of Periodic Solution for Nonlinear Second-Order Ordinary Differential Equations

3.1.3 INTRODUCTION TO DYNAMIC OPTIMIZATION: DISCRETE TIME PROBLEMS. A. The Hamiltonian and First-Order Conditions in a Finite Time Horizon

Math 334 Fall 2011 Homework 11 Solutions

Hamilton- J acobi Equation: Explicit Formulas In this lecture we try to apply the method of characteristics to the Hamilton-Jacobi equation: u t

OSCILLATION OF THIRD-ORDER FUNCTIONAL DIFFERENTIAL EQUATIONS

Variational Iteration Method for Solving System of Fractional Order Ordinary Differential Equations

Transcription:

Elecronic Journal of Differenial Equaions, Vol. 2007(2007), No. 126, pp. 1 12. ISSN: 1072-6691. URL: hp://ejde.mah.xsae.edu or hp://ejde.mah.un.edu fp ejde.mah.xsae.edu (login: fp) ASYMPTOTIC FORMS OF WEAKLY INCREASING POSITIVE SOLUTIONS FOR QUASILINEAR ORDINARY DIFFERENTIAL EQUATIONS KEN-ICHI KAMO, HIROYUKI USAMI Absrac. Asympoic forms are deermined for posiive soluions which are called weakly increasing soluions o quasilinear ordinary differenial equaions. 1. Inroducion In his paper we consider he equaion under he following condiions: ( u α 1 u ) + p() u β 1 u = 0 (1.1) (A1) α and β are posiive consans saisfying α β; (A2) p() is a C 1 funcion defined near + saisfying he asympoic condiion p() σ for some σ R as. By condiion (A2) equaion (1.1) can be rewrien in he form ( u α 1 u ) + σ (1 + ε()) u β 1 u = 0, (1.2) where ε() = σ p() 1 saisfies lim ε() = 0. Of course, here and in wha follows he symbol f() g() as means ha lim f()/g() = 1. Some preparaory resuls for equaion (1.1) are sill valid for more general equaions han (1.1); so i is convenien o consider he auxiliary equaion ( u α 1 u ) + q() u β 1 u = 0, (1.3) where we assume ha α and β saisfy condiion (A1) and q C([ 0, ); (0, )). A funcion u is defined o be a soluion of equaion (1.3) if u C 1 [ 1, ) and u α 1 u C 1 [ 1, ) and i saisfies equaion (1.3) on [ 1, ) for sufficienly large 1. I is easily seen ha all posiive soluions u() of (1.3) are classified ino he following hree ypes according as heir asympoic behavior as : (I) Asympoically linear soluion: u() c 1 for some consan c 1 > 0; (II) Weakly increasing soluion: u () 0 and u() ; (III) Asympoically consan soluion: u() c 1 for some consan c 1 > 0. 2000 Mahemaics Subjec Classificaion. 34E10, 34C41. Key words and phrases. Quasilinear ordinary differenial equaion; posiive soluion. c 2007 Texas Sae Universiy - San Marcos. Submied May 24, 2007. Published Sepember 28, 2007. 1

2 K. KAMO, H. USAMI EJDE-2007/126 Concerning qualiaive properies of posiive soluions, he sudy of asympoic behavior of asympoically linear soluions and asympoically consan soluions are raher easy, because heir firs approximaions are given by definiion. On he oher hand, we can no easily know how he weakly increasing posiive soluions behave excep in he case α = 1; see [1, 3]. In [3, Secion 20], equaion (1.1) wih α = 1 has been considered sysemaically, and asympoic forms of weakly increasing posiive soluions are given by means of he parameers β and σ. When α 1, as far as he auhors are aware, here are no works in which asympoic forms of weakly increasing posiive soluions are sudied sysemaically. Moivaed by hese facs in his paper we make an aemp o find ou asympoic forms of weakly increasing posiive soluions of (1.1) for he general case α > 0. Furhermore we will also esablish more han obained in [3] in he case α > β. In fac, some of our resuls are new even hough α = 1. To gain an insigh ino our problem, we consider he ypical equaion ( u α 1 u ) + σ u β 1 u = 0, (1.4) where σ R is a consan. Noe ha equaion (1.1) can be regarded as a perurbaion of (1.4). Equaion (1.4) has a weakly increasing posiive soluion of he form c ρ, (c > 0, 0 < ρ < 1) if and only if min{α, β} + 1 < σ < max{α, β} + 1. This soluion is uniquely given by u 0 () = Ĉk, (1.5) where k = α σ + 1 (0, 1), Ĉ = {α(1 k)k α } 1 β α. (1.6) α β From his simple observaion we can see ha asympoic forms of weakly increasing posiive soluions of (1.3) may be srongly affeced by ha of he coefficien funcion q(). Furhermore we conjecure ha weakly increasing posiive soluions u of (1.1) behave like u 0 () given by (1.5) and (1.6) if ε() is sufficienly small a. We will show ha he above conjecure is rue in many cases. In fac, we can obain he following heorems which are he main resuls of he paper: Theorem 1.1. Le α > β. (i) Suppose ha β + 1 < σ < α + 1. Then, every weakly increasing posiive soluion u of (1.1) has he asympoic form u() u 0 () as, where u 0 is given by (1.5) and (1.6). (ii) Suppose ha σ = α + 1; namely p() α 1 as. Then, every weakly increasing posiive soluion u of (1.1) has he asympoic form u() α 1 ( α α β ) α (log ) α as. Theorem 1.2. Le α < β. Suppose ha α 1 and 1/2 < k < 1 ( (α+β +2)/2 < σ < β + 1). Suppose furhermore ha eiher ε() 2 d < (1.7) or ε () d < (1.8)

EJDE-2007/126 ASYMPTOTIC FORMS 3 holds. Then, every weakly increasing posiive soluion u of (1.1) has he asympoic form u() u 0 () as, where u 0 is given by (1.5) and (1.6). Theorem 1.3. Le α < β. Suppose ha α 1 and 0 < k < 1/2( α + 1 < σ < (α + β + 2)/2). Suppose furhermore ha eiher (1.7) or (1.8) holds. Then, he same conclusion as in Theorem 1.2 holds. Remark 1.4. (i) In Theorem 1.1 he differeniabiliy of p is acually unnecessary. Similarly, in Theorems 1.2 and 1.3, he differeniabiliy of p is unnecessary when (1.7) is assumed. (ii) When α = 1 and ε() 0, Theorems 1.1, 1.2 and 1.3 were obained by [1] and [3, Corollaries 20.2, 20.3]. Remark 1.5. Le α < β. We can no prove wheher or no our conjecure is rue in he following cases: (i) α 1 and 0 < k < 1/2; (ii) α 1 and 1/2 < k < 1; and (iii) k = 1/2. We noe ha exisence resuls of weakly increasing posiive soluions o (1.3) and (1.1) are known for he case α > β. In fac, equaion (1.1) has a weakly increasing posiive soluion if and only if β + 1 < σ α + 1; see Remark 3.4 in Secion 3. In conras, i seems ha here are no such useful resuls for he case α < β. Bu we can show many concree examples of hose equaions ha have weakly increasing posiive soluions. The paper is organized as follows. In Secion 2 we give preparaory lemmas employed laer. In Secion 3 we consider equaion (1.1), as well as (1.3), under he sub-homogeneiy condiion α > β. When q() saisfie < lim inf q()/ σ lim sup q()/ σ < for some σ R, we can obain a resul which may be called as asympoic equivalence heorem for equaion (1.3); see Corollary 3.3. Theorem 1.1 is a direc consequence of his corollary. In Secion 4 we consider only equaion (1.1) under he super-homogeneiy condiion α < β, and we prove Theorems 1.2 and 1.3 here. Oher relaed resuls are found in [2, 4, 5, 6]. 2. Preparaory lemmas Lemma 2.1. Le w C 1 [ 0, ), w () = O(1) as, and w L λ [ 0, ) for some λ > 0. Then, lim w() = 0. Proof. We have w() λ w() = w( 0 ) λ w( 0 ) + = w( 0 ) λ w( 0 ) + (λ + 1) 0 ( w(s) λ w(s)) ds 0 w(s) λ w (s)ds. By our assumpions he above inegral converges. Hence lim w() λ w() exiss in R. Since w L λ [ 0, ), he limi mus be 0. The proof is complee. Lemma 2.2. Le u C 1 [ 0, ), u() > 0 and u () 0 as. Then, u () u() for sufficienly large, and he funcion u()/ is decreasing near.

4 K. KAMO, H. USAMI EJDE-2007/126 Proof. Since u() = u( 0 ) + u (s)ds u( 0 ) + u ()( 0 ), 0 we have u () u() 0 u () u( 0 ). Noing he assumpion u ( ) = 0 we find ha u () u() < 0 near. Since (u()/) = (u () u())/ 2, he proof is compleed. 3. Sub-homogeneous case: α > β Throughou he secion we assume ha α > β. As a firs sep we give he growh esimaes for weakly increasing posiive soluions of (1.3): Lemma 3.1. Le u be a weakly increasing posiive soluion of (1.3). following esimaes hold near : (α β ) α { ( ) 1/αds } α q(r)dr α 1 u() ( α β ) α { α s 1 s β/α where 1 is a sufficienly large number. ( s ) 1/αds } α r β q(r)dr Then he (3.1) Noe ha s β q(s)ds < if equaion (1.3) has a weakly increasing posiive soluion; see (ii) of Remark 3.4. Proof of Lemma 3.1. We may assume ha u, u > 0 for 1. Since u saisfies for large, and u is increasing, we have ha is u () α = u () α u() β q(s)ds, q(s)u(s) β ds, (3.2) ( 1/α. u ()u() β/α q(s)ds) (3.3) An inegraion of his inequaliy on he inerval [ 1, ] gives α } ( {u() 1/αds, α u(1 ) α q(r)dr) α β which proves he firs inequaliy of (3.1). On he oher hand, by he decreasing naure of u()/ shown in Lemma 2.2, we find from (3.2) ha Accordingly, u () α ( u() 1 ) β s β q(s)ds. u ()u() β/α β/α( 1/α. s q(s)ds) β As before we can ge he second inequaliy in (3.1). The proof is complee. s

EJDE-2007/126 ASYMPTOTIC FORMS 5 To give he main resul in his secion, le us consider he wo equaions, of he same ype, ( u α 1 u ) + q 1 () u β 1 u = 0, (3.4) ( u α 1 u ) + q 2 () u β 1 u = 0. (3.5) Here, we assume ha 0 < α < β and q 1, q 2 C([ 0, ); (0, )). Theorem 3.2. Suppose ha q 1 () q 2 () as, (3.6) ( ) 1/αds ( 1/αds C s β/α r β q 1 (r)dr q 1 (r)dr) (3.7) 0 s 0 s hold for some consan C > 0. If u 1 and u 2 are weakly increasing posiive soluions of equaions (3.4) and (3.5), respecively, hen u 1 () u 2 () as. Corollary 3.3. Suppose ha q 1 and q 2 saisfy (3.6) and 0 < lim inf q 1()/ σ lim sup q 1 ()/ σ < for some σ (β + 1, α + 1]. If u 1 and u 2 are weakly increasing posiive soluions of equaions (3.4) and (3.5), respecively, hen u 1 () u 2 () as. Theorem 1.1 is an immediae consequence of Corollary 3.3. Indeed, o see (ii) of Theorem 1.1, i suffices o noice he fac ha he equaion ( u α 1 u ) + α 1( β ) 1 u β 1 u = 0 (α β) log has a weakly increasing posiive soluion given explicily by α ( 1 α ) α (log ) α. α β Proof of Theorem 3.2. Pu z() = u 1 ()/u 2 (), 0, 0 being sufficienly large. Then, z saisfies he equaion z + 2u 2() u 2 () z + u 2() β 1 [ (u2 ()z + u α 2()z) 1 α q 1 ()z β q 2 ()u 2() 1 α z ] = 0. If z (T ) = 0 for some T, hen ( z (T ) = α 1 q 1 (T )u 2 (T ) β 1 u 2(T ) 1 α q2 (T ) z(t ) q 1 (T ) z(t )β α). Thus, if z = 0 in he region z > (q 1 ()/q 2 ()) 1/(), hen z aains a local minimum here; while if z = 0 in he region 0 < z < (q 1 ()/q 2 ()) 1/(), hen z aains a local maximum here. Noe ha by our assumpion lim (q 1 ()/q 2 ()) 1/() = 1. These simple observaions are used below. Since Lemma 3.1 and condiions (3.6) and (3.7) imply ha z() is bounded and bounded from 0, we can pu 0 < l = lim inf z() lim sup z() = L <. We claim ha l = L; ha is lim z() (0, ) exiss. Suppose for conradicion ha l L. We rea he following four cases separaely: (a)l 1 > l; (b)l > 1 l; (c)l > l 1; (d)1 L > l. Suppose ha case (a) occurs. We can find wo sequences {T n } and { n } saisfying lim n T n = lim n n = (3.8)

6 K. KAMO, H. USAMI EJDE-2007/126 and lim z(t n) = L, n lim z( n) = l, n < T n < n+1 for n = 1, 2,.... (3.9) n Since lim (q 1 ()/q 2 ()) 1/() = 1, we may assume ha z( n ) < (q 1 ( n )/q 2 ( n )) 1/(). For sufficienly large n N he minimum of z() on he inerval [T n 1, T n ] mus be aained a an inerior poin, say (T n 1, T n ). Obviously, z ( ) = 0 and z ( ) 0. However, since z( ) z( n ) for sufficienly large n, we ge a conradicion o he above observaion. Hence case (a) doeo occur. Nex suppose ha case (c) occurs. As in case (a) we can find wo sequences {T n } and { n } saisfying (3.8) and (3.9). For sufficienly lage n N he maximum of z() on he inerval [ n, n+1 ] mus be aained a an inerior poin, say ( n, n+1 ). Obviously, z ( ) = 0 and z ( ) 0. Since z( ) z(t n ) and z(t n ) > (q 1 (T n )/q 2 (T n )) 1/() for sufficienly large n, we ge a conradicion as before. Hence case (c) doeo occur. Similarly we can show ha he oher cases can no occur. Therefore lim z() = lim u 1 ()/u 2 () = m (0, ) exiss. Finally, by L Hospial s rule we have u 1 () ( m = lim u 2 () = u lim 1() α ) 1/α u 2 ( ()α [u = lim 1() α ] ) 1/α [u 2 ()α ] ( = lim q 1 ()u 1 () β q 2 ()u 2 () β ) 1/α = m β/α ; ha is m = m β/α. Since α > β, we have m = 1. This complees he proof. Remark 3.4. Concerning he exisence properies of weakly increasing posiive soluions, we know he following resuls: (i) If β q()d < ; and ( 1/αd q(s)ds) =, (3.10) Then, equaion (1.3) has weakly increasing posiive soluions [2, Example 1]. (ii) Conversely, if equaion (1.3) has a weakly increasing posiive soluion, hen we can show ha β q()d < ; and β/α( 1/αd s q(s)ds) β =. (3.11) In fac, he firs condiion in (3.11) follows from [2, Example 2]; while he second one is an immediae consequence of he esimaes in Lemma 3.1. In paricular, when α = 1, we find ha condiions (3.10) and (3.11) are he same; ha is, equaion (1.3) (wih α = 1) has a weakly increasing posiive soluion if and only if (3.10) (wih α = 1) holds.

EJDE-2007/126 ASYMPTOTIC FORMS 7 4. Super-homogeneous case: α < β Throughou his secion we assume ha α < β. In his case he siuaion seems o be more complicaed han in he previous case. The main purpose of he secion is o give he proofs of Theorems 1.2 and 1.3. To his end we need several lemmas. Lemma 4.1. Le 0 < lim inf q()/ σ lim sup q()/ σ < for some σ (α+1, β +1). Then every weakly increasing posiive soluion u of (1.1) saisfies u() = O(u 0 ()) and u () = O(u 0()) as, where u 0 is he exac soluion of (1.4) given by (1.5) and (1.6). Proof. As in he proof of Lemma 3.1 we obain (3.3). An inegraion of (3.3) on he inerval [, ) for large will give { ( 1/αds } α/(β α) u() C 1 q(r)dr) C2 u 0 (), s where C 1 and C 2 are posiive consan. Furhermore, by (3.2) we find ha ( ) 1/α ( 1/α u () = q(s)u(s) β ds C3 s ds) σ+kβ = C4 k 1 = O(u 0()) as, where C 3 and C 4 are posiive consans. This complees he proof. Lemma 4.2. Le σ (α + 1, β + 1), and u be a weakly increasing posiive soluion of equaion (1.1). Pu s = log u 0 () and v = u/u 0. Then (i) v, v = O(1) as s, and v + v > 0 near, where = d/ds; (ii) v(s) saisfieear he equaion v + a v bv + b( v + v) 1 α v β + bδ(s)( v + v) 1 α v β = 0, (4.1) where a = 2 1 k 0, b = 1 k k > 0, and δ(s) = ε(). Proof. We will prove only (i), because (ii) can be proved by direc compuaions. We noe ha u, u > 0. Since u = u 0 v, he boundedness of v follows from Lemma 4.1. Noing du/d = Ĉkk 1 (v + v), we have v + v > 0. On he oher hand, since d/ds = /k, we have v = d ( u ) d d u 0 ds This complees he proof. = u u 0 u 0u u 2 0 k C k 1 k 2k = O(1) as s. Lemma 4.3. Le he assumpion eiher of Theorem 1.2 or Theorem 1.3 hold, and v be as in Lemma 4.2. Then v L 2 [, ) for sufficienly large. Proof. We noe ha condiions (1.7) and (1.8), respecively, are equivalen o δ(s) 2 ds < (4.2) and δ(s) ds <. (4.3) We firsly consider he case where assumpions of Theorem 1.2 hold. In his case, he consan a appearing in (4.1) is posiive. We muliply he boh sides of (4.1) by v. Since α 1, we have (1 + δ(s))( v + v) 1 α v (1 + δ(s))v 1 α v; and so we obain v v + a v 2 bv v + bv 1 α+β v + bδ(s)v 1 α+β v 0. (4.4)

8 K. KAMO, H. USAMI EJDE-2007/126 An inegraion gives v 2 2 + a v 2 dr b 2 v2 + bv2 α+β 2 α + β + b δ(r)v 1 α+β vdr cons; (4.5) ha is a v 2 dr + b δ(r)v 1 α+β vdr O(1) as s. Here we have employed (i) of Lemma 4.2. Le he inegral condiion (1.7) hold; ha is, le (4.2) hold. By he Schwarz inequaliy we have ( ) 1/2 ( ) 1/2 a v 2 dr C 1 δ(r) 2 dr v 2 dr O(1) for some consan C 1 > 0. Therefore v L 2 [, ). Nex le (1.8) hold. Using inegral by pars, we obain from (4.5) v 2 2 + a v 2 dr b b[1 + 2 v2 δ(r)]v2 α+β b s + δ(r)v 2 α+β dr cons. 2 α + β 2 α + β Noing (i) of Lemma 4.2, we find ha v L 2 [, ). Secondly we consider he case where assumpions of Theorem 1.3 hold. As above, we muliply boh he sides of (4.1) by v. Since α 1, we have (1+δ(s))(v+ v) 1 α v (1 + δ(s))v 1 α v, and so we obain a v 2 v v bv v + b(1 + δ(s))v 1 α+β v. An inegraion on he inerval [, s] gives a v 2 dr v2 2 bv2 2 + bv2 α+β 2 α + β + b δ(r)v 1 α+β vdr + cons. As before, we will obain v L 2 [, ). This complees he proof. Proof of Theorem 1.2. To his end i suffices o show ha lim s v(s) = 1, where v(s) is he funcion inroduced in Lemma 4.2. The proof is divided ino hree seps. Sep 1. We claim ha lim inf s v(s) > 0; or equivalenly lim inf u()/u 0 () > 0. The proof is done by conradicion. Suppose ha lim inf s v(s) = 0. Firsly, we suppose ha v(s) decrease o 0 as s. This means ha u()/u 0 () decreases o 0 as. Accordingly we have u () α = = ( u() u 0 () p(r)u(r) β dr p(r)u 0 (r) β( u(r) ) βdr u 0 (r) ) β p(r)u 0 (r) β dr = C 1 1 σ u() β, where C 1 > 0 is a consan. Consequenly we obain he differenial inequaliy u C 2 (1 σ)/α u β/α for some consan C 2 > 0 near. Bu his differenial inequaliy implies ha u()/u 0 () v(s) C 3 > 0 for some consan C 3 > 0. This is an obvious conradicion. Nex suppose ha lim inf s v(s) = 0 and v(s) changes he sign in any neighborhood of. We noice ha, if v = 0 in

EJDE-2007/126 ASYMPTOTIC FORMS 9 he region 0 < v < [1 + δ(s)] 1/(β α), hen v > 0; while if v = 0 in he region v > [1 + δ(s)] 1/(β α), hen v < 0. Therefore, in his case he curve v = v(s) mus cross he curve v = [1 + δ(s)] 1/(β α) infiniely many imes as s. Therefore, we can find ou wo sequences {ξ n } and {η n } saisfying and ξ n < η n < ξ n+1, n = 1, 2,... ; lim n ξ n = lim n η n = v(η n ) 0 a, v(ξ n ) = [1 + δ(ξ n )] 1 β α 1 a. An inegraion of (4.4) on [ξ n, η n ] yields 1 2 { v(η n) 2 v(ξ n ) 2 } + a + ηn ξ n v 2 dr b 2 {v(η n) 2 v(ξ n ) 2 } b 2 α + β {v(η n) 2 α+β v(ξ n ) 2 α+β } + b ηn ξ n δ(r)v 1 α+β vdr 0. (4.6) From equaion (4.1) and (i) of Lemma 4.2 we know ha v = O(1) as s. This fac and he fac ha v L 2 [, ) imply ha lim s v(s) = 0 by Lemma 2.1. Accordingly (4.6) is equivalen o o(1) + o(1) b b (o(1) 1) + (o(1) 1) + o(1) 0 as s. 2 2 α + β Leing n, we ge b/2 b/(2 α + β) 0 a conradicion o he assumpion β > α. Therefore, lim inf s v(s) > 0. Sep 2. We claim ha here is a limi lim s v(s) (0, ). To see his, we inegrae (4.1) muliplied by v: v 2 2 + a + b v 2 dr b 2 v2 + b ( v + v) 1 α v β vdr δ(r)( v + v) 1 α v β vdr = cons. (4.7) Suppose ha condiion (1.7) holds; or equivalenly (4.2) holds. Since v L 2 [, ), he firs, and he hird inegrals in he lef hand side of (4.7) converge as s. The mean value heorem shows ha (v + v) 1 α = ( 1 + v v ) 1 αv 1 α = v 1 α + (1 α) (v + θ(r) v) α v, (4.8) where θ(r) is a quaniy saisfying 0 < θ(r) < 1. Therefore, ( v + v) 1 α v β vdr = {v 1 α+β v + (1 α)(v + θ(r) v) α v β v 2 }dr = v(s)2+β α 2 + β α + O(1) v 2 dr + cons. So we find ha he funcion v 2 /2+v 2+β α /(2+β α) has a finie limi. This fac shows ha lim s v(s) = m (0, ) exiss. Suppose ha (1.8) or equivalenly

10 K. KAMO, H. USAMI EJDE-2007/126 (4.3) holds. By (4.8), we have = δ(r)( v + v) 1 α v β vdr {δ(r)v 1 α+β v + δ(r)(1 α)(v + θ(r) v) α v β v 2 }dr = δ(s)v2+β α 2 + β α 1 2 + β α δ(r)v 2+β α dr + cons + O(1) v 2 dr as s. Hence, as before we know ha he funcion v 2 /2 + v 2+β α /(2 + β α) has a finie limi. Therefore m = lim s v(s) (0, ) exiss. Sep 3. Finally, we le s in equaion (4.1). Then, we have lim s v(s) = b(m m 1+β α ). Since v = o(1), we mus have lim s v(s) = 0, implying m = 1. The proof of Theorem 1.2 is complee. Proof of Theorem 1.3. Firsly we show ha lim inf s v(s) > 0. The proof is done by conradicion. Suppose ha lim inf s v(s) = 0. We may assume ha v changes he sign in any neighborhood of, because he case in which v decreases o 0 can be reaed as in he proof of Theorem 1.2 (Sep 1). Since v(s) akes local maxima in he region v (1+δ(s)) 1/(β α), here are he following sequences { } and { } saisfying v( ) = v( ) = 0, < < +1, lim = lim =, n n lim v( ) = 0, v() (1 + δ( )) 1/(β α). n Now, we decompose α in he form α = m ρ, where m N and ρ > 0. Alhough here are infiniely many such choices of decomposiion for α, we fix one choice for a momen. We rewrie equaion (4.1) as v a v bv + b( v + v) m+1+ρ v β + bδ(s)( v + v) m+1+ρ v β = 0. We muliply boh he sides by (v + v) m v and hen inegrae he resuling equaion on he inerval [, ] o obain + b v v(v + v) m dr a (v + v) 1+ρ vv β dr + b (v + v) m v 2 dr b v v(v + v) m dr δ(r)(v + v) 1+ρ vv β dr = 0. (4.9) The binomial expansion implies m c k v v k+1 v m k dr a k=0 + b (v + v) 1+ρ vv β dr + b (v + v) m v 2 dr b k=0 δ(r)(v + v) 1+ρ vv β dr = 0, m c k v m k+1 v k+1 dr

EJDE-2007/126 ASYMPTOTIC FORMS 11 where c k = ( ) m k are he binomial coefficiens. Now, we evaluae each erm in he lef hand side. For k {0, 1,..., m 1} we obain v v k+1 v m k dr = = m k k + 2 d ( v k+2 ) v m k dr dr k + 2 v k+3 v m k 1 dr = o(1) a. For k = m obviously we have v v k+1 dr = 0. Hence he firs erm of he lef hand side of (4.9) ends o 0 a. The second erm is dominaed by cons v 2 dr, and hence i ends o zero a. Nex, we compue he hird erm. For k {1, 2,..., m} we have have v m+1 vdr = 1 m + 2 Therefore, he hird erm is equal o v m k+1 v k+1 dr cons v 2 dr. For k = 0, we ( v(sn ) m+2 v( ) m+2) = v() m+2 + o(1) a. m + 2 o(1) bv() m+2 a. m + 2 To evaluae he fourh erm we employ he mean value heorem o obain (v + v) 1+ρ = v 1+ρ + (1 + ρ) (v + θ(r) v) ρ v, where θ(r) is a quaniy beween 0 and 1. Hence we can compue = (v + v) 1+ρ vv β dr v 1+ρ+β vdr + (1 + ρ) = v() 2+ρ+β v( ) 2+ρ+β 2 + ρ + β (v + θ(r) v) ρ v 2 v β dr + (1 + ρ) O(1) v 2 dr = v() 2+ρ+β + o(1) a. 2 + ρ + β Finally by Schwarz s inequaliy we find ha he las erm is dominaed by he quaniy ( ) 1/2 ( ) 1/2 cons δ(r) 2 dr v 2 dr = o(1) a. (Noe ha (1.7) or equivalenly (4.2) is assumed.) Consequenly, from (4.9) we obain he formula o(1) b m + 2 v() m+2 b + 2 + ρ + β v() 2+ρ+β + o(1) = 0 a. This implies ha lim n v( ) = [(m + 2 + β α)/(m + 2)] 1/(β α). Since m can be moved arbirarily, his is an obvious conradicion. Therefore lim inf s v > 0. We are now in a posiion o show lim s v(s) = 1. Since lim inf s v(s) > 0, we find ha lim inf u()/u 0 () > 0. Inegraing equaion (3.2) (wih q replaced by p), we furher find ha lim inf u ()/u 0() > 0. Since v + v = u ()/u 0(), we

12 K. KAMO, H. USAMI EJDE-2007/126 obain lim inf s (v + v) > 0. Recalling equaion (4.1), we find ha v(s) = O(1) as s. Since we have already shown ha v L 2 [, ), Lemma 2.1 shows ha lim s v = 0. Consequenly, as in he proof of Theorem 1.2 we can prove ha lim s v(s) = 1. This complees he proof of Theorem 1.3. References [1] R. Bellman, Sabiliy heory of differenial equaions, MaGraw-Hill, New York, 1953. (Reprin: Dover Publicaions, Inc., 1969) [2] Á. Elber and T. Kusano, Oscillaion and non-oscillaion heorems for a class of second order quasilinear differenial equaions, Aca Mah. Hung. 56 (1990), 325-336. [3] I. T. Kiguradze and T. A. Chanuria, Asympoic properies of soluions of nonauonomous ordinary differenial equaions, Kluwer Academic Publisher, Dordrech, 1992. [4] M. Kiano and T. Kusano, On a class of second order quasilinear ordinary differenial equaions, Hiroshima Mah. J. 25 (1995), 321-355. [5] R. A. Moore and Z. Nehari, Nonoscillaion heorems for a class of nonlinear differenial equaions, Trans. Amer. Mah. Soc. 93 (1959), 30-52. [6] K. Nishihara, Asympoic behaviors of soluions of second order differenial equaions, J. Mah. Anal. Appl. 189 (1995), 424-441. Ken-ichi Kamo Division of Mahemaics, School of Medicine, Liberal Ars and Sciences, Sapporo Medical Universiy, S1W17, Chuoku, Sapporo 060-8543, Japan E-mail address: kamo@sapmed.ac.jp Hiroyuki Usami Deparmen of Mahemaics, Graduae School of Science, Hiroshima Universiy, Higashi - Hiroshima, 739-8521, Japan E-mail address: usami@mis.hiroshima-u.ac.jp