Some properties of solutions of the homogeneous nonlinear second order differential equations

Abstract

In this paper we consider the following nonlinear homogeneous second order differential equations, \(F(x,y,y^{\prime},y^{\prime\prime})=0.\) We present for the solutions, \(y\in C^2[a,b]\), of this equation, extremal principle, Sturm-type, Nicolescu-type and Butlewski-type separation theorems.

Some applications and examples are given. Open problems are also presented.

Authors

V. Ilea
(Babes Bolyai Univ)

D. Otrocol
(Tiberiu Popoviciu Institute of Numerical Analysis, Romanian Academy)

I.A. Rus
(Babes Bolyai Univ.)

Keywords

Homogeneous nonlinear second order differential equation, zeros of solutions, Sturm-type theorem, Nicolescu-type theorem, Butlewski-type theorem, bilocal problem, Cauchy problem, open problem, extremal principle.

Cite this paper as:

V. Ilea, D. Otrocol, I. A. Rus, Some properties of solutions of the homogeneous nonlinear second order differential equations, Mathematica, 57 (80) (2015), no 1-2, pp. 38-43

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2016-Ilea-Otrocol-Rus-Some properties of solutions.pdf ??

About this paper

Journal

Mathematica

Publisher Name

Romanian Academy Publishing House

Print ISSN

1222-9016

Online ISSN

2601-744X

MR

MR3611700

ZBL

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Some properties of solutions of the homogeneous nonlinear second order differential equations

VERONICA ILEA , DIANA OTROCOL and IOAN A. RUS
Abstract.

In this paper we consider the following nonlinear homogeneous second order differential equations, F(x,y,y,y′′)=0.F(x,y,y^{\prime},y^{\prime\prime})=0. We present for the solutions, yC2[a,b]y\in C^{2}[a,b], of this equation, extremal principle, Sturm-type, Nicolescu-type and Butlewski-type separation theorems. Some applications and examples are given. Open problems are also presented.

1. Introduction

Let FC([a,b]×3).F\in C([a,b]\times\mathbb{R}^{3}). We consider the following implicit differential equation

(1.1) F(x,y,y,y′′)=0.F(x,y,y^{\prime},y^{\prime\prime})=0.

By definition this equation is homogeneous if the function FF is homogeneous with respect to the last three arguments.

In this paper by a solution of the equation (1.1) we understand a function yC2[a,b]y\in C^{2}[a,b] which satisfies (1.1). Moreover by a solution we shall understand a nontrivial solution.

The linear case of (1.1) is the following equation

(1.2) y′′+p(x)y+q(x)y=0.y^{\prime\prime}+p(x)y^{\prime}+q(x)y=0.

For the equation (1.2) the following properties of the solution are well known (see [10], [11], [12], [7], [3], [13]).

We suppose that pp and qC[a,b].q\in C[a,b].

Theorem 1.

(Extremal principle) Let q(x)<0,q(x)<0, for all x]a,b[x\in]a,b[ and yy be a solution of (1.2). Then

  • (a)

    if max{y(x)|x[a,b]}=y(x0)\max\{y(x)|\ x\in[a,b]\}=y(x_{0}) and y(x0)>0y(x_{0})>0 then x0{a,b};x_{0}\in\{a,b\};

  • (b)

    if min{y(x)|x[a,b]}=y(x0)min\{y(x)|\ x\in[a,b]\}=y(x_{0}) and y(x0)<0y(x_{0})<0 then x0{a,b}.x_{0}\in\{a,b\}.

Theorem 2.

(Sturm’s separation theorem) If y1y_{1} and y2y_{2} are two linear independent solutions of (1.2), then the zeros of y1y_{1} and y2y_{2} separate each other.

Theorem 3.

(Nicolescu’s theorem, [6]) We suppose that q(x)>0,q(x)>0, for all x[a,b].x\in[a,b]. If yy is a solution of (1.2), then the zeros of yy and yy^{\prime} separate each other.

Theorem 4.

(Butlewski’s theorem, [1]) We suppose that q(x)>0,q(x)>0, for all x[a,b].x\in[a,b]. If y1y_{1} and y2y_{2} are two linear independent solutions of (1.2), the zeros of y1y_{1}^{\prime} and y2y_{2}^{\prime} separate each other.

The aim of this paper is to extend the above results to the solutions of (1.1). For some results in this directions see [14], [8] and [9].

2. Homogeneous nonlinear second order differential equation: Examples

Example 1.

The equation

(2.1) y′′2+yy′′+y2=0y^{\prime\prime 2}+yy^{\prime\prime}+y^{2}=0

has the only solution y=0y=0.

Example 2.

We consider the equation

(2.2) y′′3+y3=0.y^{\prime\prime 3}+y^{3}=0.

This equation is equivalent with the equation y′′+y=0.y^{\prime\prime}+y=0.

Example 3.

We consider the equation

(2.3) y′′3y3=0.y^{\prime\prime 3}-y^{3}=0.

This equation is equivalent with the equation y′′y=0.y^{\prime\prime}-y=0.

Example 4.

We consider the equation

(2.4) y′′2y2=0.y^{\prime\prime 2}-y^{2}=0.

A function yy is a solution of this equation if and only if yy is a solution of y′′y=0y^{\prime\prime}-y=0 or of y′′+y=0.y^{\prime\prime}+y=0.

Example 5.

(Painlevé (1902), see [4], 6.122). The following equation was studied by Painlevé

(2.5) yy′′y2+p(x)yy+q(x)y2=0.yy^{\prime\prime}-y^{\prime 2}+p(x)yy^{\prime}+q(x)y^{2}=0.
Example 6.

(Tonelli (1927), [14]). The following equation was considered by Tonelli

(2.6) (y2+y2)y′′+p(x)y3=0.(y^{2}+y^{\prime 2})y^{\prime\prime}+p(x)y^{3}=0.
Example 7.
(2.7) k=1m(y′′+pk(x)y+qk(x)y)=0\textstyle\prod\limits_{k=1}^{m}(y^{\prime\prime}+p_{k}(x)y^{\prime}+q_{k}(x)y)=0

We shall use the above examples to exemplify our general results.

For other examples of such equations see [4] and [12].

3. Extremal principles

We consider the equation (1.1) with FC([a,b]×3)F\in C([a,b]\times\mathbb{R}^{3}) a homogeneous function with respect to the last three arguments. We have the following extremal principle.

Theorem 5.

We suppose that F(x,r1,0,r2)0,F(x,r_{1},0,r_{2})\neq 0, for all x[a,b],r1>0x\in[a,b],r_{1}>0 and r20.r_{2}\leq 0. Let yy be a solution of (1.1). We have:

  • (a)

    if max{y(x)|x[a,b]}=y(x0)\max\{y(x)|\ x\in[a,b]\}=y(x_{0}) and y(x0)>0y(x_{0})>0 then x0{a,b};x_{0}\in\{a,b\};

  • (b)

    if min{y(x)|x[a,b]}=y(x0)min\{y(x)|\ x\in[a,b]\}=y(x_{0}) and y(x0)<0y(x_{0})<0 then x0{a,b}.x_{0}\in\{a,b\}.

  • (a)

    Let x0]a,b[x_{0}\in]a,b[ be such that, y(x0)>0y(x_{0})>0 is the maximum value of yy on [a,b][a,b]. Since yC2[a,b]y\in C^{2}[a,b] we have that y(x0)>0,y(x0)=0,y′′(x0)0y(x_{0})>0,y^{\prime}(x_{0})=0,y^{\prime\prime}(x_{0})\leq 0. From (1.1) we have

    F(x0,y(x0),0,y′′(x0))=0.F(x_{0},y(x_{0}),0,y^{\prime\prime}(x_{0}))=0.

    But in the condition of our theorem the first part of this relation is not equal to zero. So, x0{a,b}.x_{0}\in\{a,b\}.

  • (b)

    We remark that if yy is a solution of (1.1) then, y-y is also a solution. We apply (a)(a) for y-y.

Example 8.

We consider the equation

(3.1) y′′2n+1+p(x)y2n+1+q(x)y2n+1=0,x[a,b] with n.y^{\prime\prime 2n+1}+p(x)y^{\prime 2n+1}+q(x)y^{2n+1}=0,\ x\in[a,b]\text{ with }n\in\mathbb{N}.

If q(x)<0,x]a,b[q(x)<0,\forall x\in]a,b[, then we have for the solution of the equation (3.1) the extremal principle given by Theorem 5.

Remark 1.

If pk,qkC[a,b]p_{k},q_{k}\in C[a,b] and qk(x)<0,x[a,b]q_{k}(x)<0,\ \forall x\in[a,b] and k=1,m¯k=\overline{1,m}, then the equation (7) satisfies the conditions of Theorem 5.

Now let us consider the bilocal problem

(1.1) F(x,y,y,y′′)=0,F(x,y,y^{\prime},y^{\prime\prime})=0,
(3.2) y(a)=0,y(b)=0.y(a)=0,y(b)=0.

We have for this problem the following result.

Theorem 6.

We suppose that F(x,r1,0,r2)0F(x,r_{1},0,r_{2})\neq 0, for all x[a,b],r1>0x\in[a,b],r_{1}>0 and r20r_{2}\leq 0. Then the problem (1.1)-(3.2) has the only solution y=0y=0.

Follows from Theorem 5. ∎

4. Zeros of the solution of (1.1)

Now we consider the following conditions on (1.1):

  • (u0)

    If yy is a solution of (1.1) and for some x0[a,b],y(x0)=0x_{0}\in[a,b],\ y(x_{0})=0 and y(x0)=0,y^{\prime}(x_{0})=0, then y=0y=0.

  • (u1)

    If y1y_{1} and y2y_{2} are solutions of (1.1) and for some x0[a,b],y1(x0)=y2(x0)>0x_{0}\in[a,b],\ y_{1}(x_{0})=y_{2}(x_{0})>0 and y1(x0)=y2(x0),y_{1}^{\prime}(x_{0})=y_{2}^{\prime}(x_{0}), then y1=y2y_{1}=y_{2}.

  • (u2)

    If yy is a solution of (1.1) and for some x0[a,b],y(x0)=0x_{0}\in[a,b],\ y^{\prime}(x_{0})=0, y′′(x0)=0,y^{\prime\prime}(x_{0})=0, then y=0y=0.

  • (u3)

    If y1y_{1} and y2y_{2} are solutions of (1.1) and for some x0[a,b],y1(x0)=y2(x0)>0x_{0}\in[a,b],\ y_{1}^{\prime}(x_{0})=y_{2}^{\prime}(x_{0})>0 and y1′′(x0)=y2′′(x0),y_{1}^{\prime\prime}(x_{0})=y_{2}^{\prime\prime}(x_{0}), then y1=y2y_{1}=y_{2}.

By standard arguments we have

Lemma 1.

If yy is a solution of (1.1) then condition (u0) implies that the zeros of yy are simple and isolated on [a,b].[a,b].

Lemma 2.

If yy is a solution of (1.1) then condition (u2) implies that the zeros of yy^{\prime} are simple and isolated on [a,b].[a,b].

In what follow we also need the following result (see [14], [10], p. 163 and [5]).

Lemma 3.

(Tonelli’s Lemma) Let y1,y2C1[a,b]y_{1},y_{2}\in C^{1}[a,b] be two functions which satisfy the following conditions:

  • (i)

    y1(a)=y1(b)=0y_{1}(a)=y_{1}(b)=0 and y1(x)>0y_{1}(x)>0 for all x]a,b[;x\in]a,b[;

  • (ii)

    y2(x)>0y_{2}(x)>0 for all x[a,b].x\in[a,b].

Then there exists λ>0\lambda>0 and x0]a,b[x_{0}\in]a,b[ such that:

y2(x0)=λy1(x0) and y2(x0)=λy1(x0).y_{2}(x_{0})=\lambda y_{1}(x_{0})\text{ and }y_{2}^{\prime}(x_{0})=\lambda y_{1}^{\prime}(x_{0}).

Using Lemma 3, Tonelli give in [14] the following result.

Theorem 7.

(Sturm-type separation theorem) For the homogeneous equation (1.1) we suppose that it satisfies conditions (u0) and (u1). Then if y1,y2y_{1},y_{2} are two linear independent solutions of (1.1) and x1,x2[a,b]x_{1},x_{2}\in[a,b] are two consecutive zeros of y1y_{1}, then y2y_{2} has at least one zero in [x1,x2][x_{1},x_{2}].

Our results are the following.

Theorem 8.

(Nicolescu-type separation theorem) For the homogeneous equation (1.1), we suppose that:

  • (i)

    it satisfies condition (u2);

  • (ii)

    F(x,λ2,λ,1)0,F(x,\lambda^{2},\lambda,1)\neq 0, for all λ.\lambda\in\mathbb{R}.

Then, if yy is a solution of (1.1), the zeros of yy and yy^{\prime} separate each other.

We consider x1x_{1} and x2x_{2} two consecutive zeros of y(x)y^{\prime}(x). We have to prove that y(x)y(x) has at least one zero in the interval (x1,x2)(x_{1},x_{2}).

We suppose that y(x)0,x[x1,x2]y(x)\neq 0,\ x\in[x_{1},x_{2}]. Applying Tonelli’s Lemma 3 there exists x0(x1,x2)x_{0}\in(x_{1},x_{2}) and λ>0(\lambda>0\ ( or <0)<0) such that

y(x0)=λy(x0),y(x0)=λy′′(x0).y(x_{0})=\lambda y^{\prime}(x_{0}),\ y^{\prime}(x_{0})=\lambda y^{\prime\prime}(x_{0}).

So,

(4.1) y(x0)=1λy(x0),y′′(x0)=1λ2y(x0).y^{\prime}(x_{0})=\tfrac{1}{\lambda}y(x_{0}),\ y^{\prime\prime}(x_{0})=\tfrac{1}{\lambda^{2}}y(x_{0}).

Using (4.1) in F(x0,y(x0),y(x0),y′′(x0))=0F(x_{0},y(x_{0}),y^{\prime}(x_{0}),y^{\prime\prime}(x_{0}))=0 we obtain that (y(x0)0y(x_{0})\neq 0)

F(x,λ2,λ,1)=0, for all λ.F(x,\lambda^{2},\lambda,1)=0,\text{ for all }\lambda\in\mathbb{R}.

Remark 2.

Theorem 8 improves Theorem 2 in [8].

Remark 3.

Theorem 8 works for the equation (7) if pk,qkC[a,b]p_{k},q_{k}\in C[a,b] and qk(x)<0,x[a,b]q_{k}(x)<0,\ \forall x\in[a,b]. It also works for the equation (3).

Theorem 9.

(Butlewski-type separation theorem) For the homogeneous equation (1.1), we suppose that it satisfies conditions (u2) and (u3). Then, if y1y_{1} and y2y_{2} are two linear independent solutions of (1.1) and x1,x2[a,b]x_{1},x_{2}\in[a,b] are two consecutive zeros of y1y_{1}^{\prime}, then y2y_{2}^{\prime} has at least one zero in [x1,x2][x_{1},x_{2}].

We consider x1x_{1} and x2x_{2} two consecutive zeros of y1(x)y_{1}^{\prime}(x). We have to prove that y2(x)y_{2}^{\prime}(x) has at least one zero in [x1,x2][x_{1},x_{2}].

We suppose that y2(x)0,x[x1,x2]y_{2}^{\prime}(x)\neq 0,\ x\in[x_{1},x_{2}]. Applying Tonelli’s Lemma 3 there exists x0(x1,x2)x_{0}\in(x_{1},x_{2}) and λ>0(\lambda>0\ ( or <0)<0) such that

y2(x0)=λy1(x0),y2′′(x0)=λy1′′(x0).y_{2}^{\prime}(x_{0})=\lambda y_{1}^{\prime}(x_{0}),\ y_{2}^{\prime\prime}(x_{0})=\lambda y_{1}^{\prime\prime}(x_{0}).

Taking into account (u2) we have that y2(x)=λy1(x)y_{2}(x)=\lambda y_{1}(x) and so we have reached a contradiction. ∎

5. Some research directions

Problem 1.

To give sufficient conditions which imply conditions (u0) and (u1).

Problem 2.

To give sufficient conditions which imply conditions (u2) and (u3).

Problem 3.

In [2] the authors studied the following problem. Let us consider the equation

L(y):=y′′+q(x)y=0L(y):=y^{\prime\prime}+q(x)y=0

with qC[a,b]q\in C[a,b]. The problem is to study the functional h:KerL+h:KerL\rightarrow\mathbb{R}_{+} defined by h(y):=inf{d(x1,x2)|x1h(y):=\inf\{d(x_{1},x_{2})|\ x_{1} and x2x_{2} are two consecutive zeros of y}.y\}. In [2] the authors prove that

inf{h(y)|yKerL}=min{h(y)|yKerL}>0.\inf\{h(y)|\ y\in KerL\}=\min\{h(y)|\ y\in KerL\}>0.

The problem is to study the above problem for the equation (1.1).

Acknowledgement 1.

The work of the first author was partially supported by a grant of the Romanian National Authority for Scientific Research, CNCS – UEFISCDI, project number PN-II-ID-PCE-2011-3-0094.

References

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Received October 15, 2000
Accepted February 20, 2001

“Babeş-Bolyai” University
Faculty of Mathematics and Computer Science
M. Kogălniceanu St., No. 1, RO-400084 Cluj-Napoca, Romania
E-mail: vdarzu@math.ubbcluj.ro
E-mail: iarus@math.ubbcluj.ro
“T Popoviciu” Institute of Numerical Analysis, Romanian Academy
P.O.Box. 68-1, 400110, Cluj-Napoca, Romania
E-mail: dotrocol@ictp.acad.ro
2015

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