Skip to main content

Oscillation and nonoscillation for second order neutral dynamic equations with positive and negative coefficients on time scales

Abstract

We investigate oscillation and nonoscillation of certain second order neutral dynamic equations with positive and negative coefficients. We apply the results from the theory of lower and upper solutions for related dynamic equations along with some additional estimates on positive solutions and use different techniques to obtain some oscillatory theorems. Also, we apply Kranoselskii’s fixed point theorem to obtain nonoscillatory results and then give two sufficient and necessary conditions for the equations to be oscillatory. Some interesting examples are given to illustrate the versatility of our results.

1 Introduction

In this paper, we investigate oscillation and nonoscillation of second order neutral functional dynamic equations with positive and negative coefficients of the form

[ p ( t ) ( x ( t ) + r ( t ) x ( g ( t ) ) ) Δ ] Δ +h ( t , x σ ( t ) , x ( τ 1 ( t ) ) , x ( τ 2 ( t ) ) , x ( ξ 1 ( t ) ) , x ( ξ 2 ( t ) ) ) =0,
(1.1)

where tT, hC(T× R 1 + 2 + 2 ,R), Φ γ (u)= | u | γ 1 u, γ>0,

h ( t , x 0 , x 1 , x 2 , x 3 , x 4 ) = q 0 ( t ) Φ γ ( x 0 ) + q 1 ( t ) Φ γ ( x 1 ) q 2 ( t ) Φ γ ( x 2 ) + s 1 ( t ) Φ γ ( x 3 ) s 2 ( t ) Φ γ ( x 4 ) .
(1.2)

Throughout this paper, we shall assume that T is a time scale satisfying infT= t 0 and supT=, and

(B1) p C rd ( [ t 0 , ) T ,(0,)) satisfies t 0 1 p ( s ) Δs=;

(B2) there exists a constant r 0 , 0 r 0 <1 such that r C rd (T,[0, r 0 ]);

(B3) g C rd ( T , T ), g(t)t, lim t g(t)=;

(B4) τ 1 , τ 2 C rd ( T , T ) are injective, τ 1 (t) τ 2 (t)t, lim t τ 1 (t)= and Im τ 1 (T)Im τ 2 (T);

(B5) ξ 1 , ξ 2 C rd ( T , T ) are injective, ξ 1 (t) ξ 2 (t)σ(t), and for sufficiently large T 0 T, there exists T 0 T such that ξ 1 ( T 0 )= ξ 2 ( T 0 ) and A 1 ={Im ξ 1 (t):t T 0 } A 2 ={Im ξ 2 (t):t T 0 };

(B6) q 0 (t), q 1 (t), q 2 (t), s 1 (t), s 2 (t) C rd (T,R) are eventually positive, and satisfy

q 1 ( τ 1 1 ( τ 2 ( t ) ) ) q 2 ( t ) , s 1 ( ξ 1 1 ( ξ 2 ( t ) ) ) s 2 ( t ) , q 0 ( σ 1 ( ξ 2 ( t ) ) ) s 2 ( t ) , q 0 ( σ 1 ( τ 1 ( t ) ) ) q 2 ( t ) .

A solution x(t) of (1.1) is said to be oscillatory if it is neither eventually positive nor eventually negative, otherwise it is nonoscillatory. The equation itself is called oscillatory if all its solutions are oscillatory.

In recent years, there has been an increasing interest in studying the oscillation and nonoscillation of solutions of dynamic equations on time scales since Hilger introduced the theory of time scale which was excepted to unify continuous and discrete calculus. We refer the readers to the monographs [14], the papers [3, 517] and the references cited therein.

The results on oscillation of dynamic equations with positive and negative coefficients are mainly concentrated on differential equations or difference equations. To the best of our knowledge, there are few researches on dynamic equations with positive and negative coefficients on time scales. In [13], Özbekler and Zafer gave new oscillation criteria for superlinear and sublinear forced dynamic equations with positive and negative coefficients by means of nonprinciple solutions. Also, Özbekler et al. [14] made use of the concept of nonprinciple solutions to establish new oscillation criteria. However, in general, it is difficult for us to find a nonprinciple solution of second order dynamic equations. As a result, their approach may be difficult to apply to second order dynamic equations. Under the convergence of double integral of negative coefficients, sufficient conditions for oscillation was given in [12, 1618]. The results on oscillation of difference equations with positive and negative coefficients can be found in [8, 15] and references therein.

In this paper, to obtain oscillatory theorems, we shall apply results from the theory of lower and upper solutions for related dynamic equations along with some additional estimates on positive solutions and use some different techniques. Also, we apply Kranoselskii’s fixed point theorem to obtain nonoscillatory results and then give two sufficient and necessary conditions for (1.1) being oscillatory. Our results cannot only be applied to differential equations and difference equations, but they can also be applied to other dynamic equations with positive and negative coefficients.

In Section 2, we present some preliminaries and important estimates, especially the estimate z Δ (t)0 and the function h>0 if the solution x(t)>0 of (1.1). In Section 3, we give several oscillatory and nonoscillatory results. In Section 4, we illustrate the versatility of our results by three examples.

2 Some preliminaries

In order to prove our main results, we establish some fundamental results in this section. Now we introduce the auxiliary functions

P(t,a)= a t Δ s p ( s ) , η i (t,a)= P ( τ i ( t ) , a ) P ( σ ( t ) , a ) , ν j (t,a)= P ( ξ j ( t ) , a ) P ( σ ( t ) , a ) ,
(2.1)

where 1in, 1jm, a [ t 0 , ) T . For the convenience of discussion, let

z(t)=x(t)+r(t)x ( g ( t ) ) .

Let m 1 =1 r 0 . Furthermore, we need the following additional hypotheses:

q 0 (t) Φ γ ( m 1 ) q 2 (t)0, s 1 (t) Φ γ ( m 1 ) s 2 (t)0
(2.2)

or

s 1 (t) Φ γ ( m 1 ) q 2 (t) s 2 (t)0.
(2.3)

First of all, we give the following estimates.

Lemma 2.1 Assume that conditions (B1)-(B6) and one of (2.2)-(2.3) hold. Let x(t) be an eventually positive solution of equation (1.1). Then there exists some T t 0 such that

  1. (i)

    for all tT, z(t)>0, z Δ (t)>0, x(t)(1r(t))z(t), and

    h ( t , x σ ( t ) , x ( τ 1 ( t ) ) , x ( τ 2 ( t ) ) , x ( ξ 1 ( t ) ) , x ( ξ 2 ( t ) ) ) >0;
  2. (ii)

    for each 1i2, 1j2 and for ξ j (t)σ(t)t τ i (t)T, we have

    z ( τ i ( t ) ) η i (t,T) z σ (t)andz ( ξ j ( t ) ) ν j (t,T) z σ (t);
  3. (iii)

    if p(t) is nondecreasing, each 1i2, 1j2 and for ξ j (t)σ(t)t ξ j (T) τ i (t)T, we have

    z ( τ i ( t ) ) z σ ( t ) τ i ( t ) τ i ( T ) σ ( t ) τ i ( T ) and z ( ξ j ( t ) ) z σ ( t ) ξ j ( t ) ξ j ( T ) σ ( t ) ξ j ( T ) .

Proof (i) Suppose that x(t) is an eventually positive solution of (1.1). In view of conditions (B2)-(B6), there exists T 1 T such that x(t)>0, x(g(t))>0, x( τ i (t))>0, 1i2, x( ξ j (t))>0, 1j2, and 0r(t) r 0 <1 for all t [ T 1 , ) T . It is immediate to obtain z(t)0 by z(t)=x(t)+r(t)x(g(t)).

Next, we show that z Δ (t) is eventually positive. Otherwise there exists a sequence { t n } n = 1 with lim l t l = such that z Δ ( t i )<0 and τ 1 1 ( τ 2 ( t l )) t l for some lN. Without loss of generality, we may assume that l=1, i.e. τ 1 1 ( τ 2 ( t 1 )) t 1 . For t τ 2 1 ( τ 1 (t)) ξ 2 1 ( ξ 1 ( t 1 )) t 1 and t ξ 1 1 ( ξ 2 (t)), let

{ D 1 = t 1 t q 0 ( s ) Φ γ ( x σ ( s ) ) Δ s + τ 2 1 ( τ 1 ( t ) ) t q 2 ( s ) Φ γ ( x ( τ 2 ( s ) ) ) Δ s D 1 = + t 1 ξ 2 1 ( ξ 1 ( t 1 ) ) s 2 ( s ) Φ γ ( x ( ξ 2 ( s ) ) ) Δ s , D 2 = t 1 t q 1 ( s ) Φ γ ( x ( τ 1 ( s ) ) ) Δ s + t 1 τ 2 1 ( τ 1 ( t ) ) q 2 ( s ) Φ γ ( x ( τ 2 ( s ) ) ) Δ s , D 3 = t 1 t s 1 ( s ) Φ γ ( x ( ξ 1 ( s ) ) ) Δ s + ξ 2 1 ( ξ 1 ( t 1 ) ) t s 2 ( s ) Φ γ ( x ( ξ 2 ( s ) ) ) Δ s .

We rewrite D 2 as follows:

D 2 = t 1 τ 1 1 ( τ 2 ( t 1 ) ) q 1 ( s ) Φ γ ( x ( τ 1 ( s ) ) ) Δ s τ 1 1 ( τ 2 ( t 1 ) ) t q 1 ( s ) Φ γ ( x ( τ 1 ( s ) ) ) Δ s + t 1 τ 2 1 ( τ 1 ( t ) ) q 2 ( s ) Φ γ ( x ( τ 2 ( s ) ) ) Δ s .

By (B6), we see that q 1 ( τ 1 1 ( τ 2 (t))) q 2 (t) and then clearly D 2 0. Similarly, we also have D 1 0 and D 3 0.

Then, for t τ 2 1 ( τ 1 (t)) ξ 2 1 ( ξ 1 ( t 1 )) t 1 and t ξ 1 1 ( ξ 2 (t)), integrating (1.1) from t 1 to t, by (B1)-(B6) and the geometric sense of a definite integral, we obtain

p ( t ) z Δ ( t ) p ( t 1 ) z Δ ( t 1 ) = t 1 t h ( s , x σ ( s ) , x ( τ 1 ( s ) ) , x ( τ 2 ( s ) ) , x ( ξ 1 ( s ) ) , x ( ξ 2 ( s ) ) ) Δ s = D 1 + D 2 + D 3 0 .

It follows that

z(t)z( t 1 )p( t 1 ) z Δ ( t 1 ) t 1 t Δ s p ( s ) as t,

which contradicts z(t)=x(t)+r(t)x(g(t))>0.

Since x(t) is a solution of (1.1) satisfying x(t)>0 and z Δ (t)>0, we see that

x(t)=z(t)r(t)x ( g ( t ) ) z(t)r(t)z ( g ( t ) ) z(t)r(t)z(t)= ( 1 r ( t ) ) z(t).

Now, we claim that h(t, x σ (t),x( τ 1 (t)),x( τ 2 (t)),x( ξ 1 (t)),x( ξ 2 (t)))>0. By (2.2) or (2.3), x(t)(1r(t))z(t) and z Δ (t)0 for t T 1 , we have

h ( t , x σ ( t ) , x ( τ 1 ( t ) ) , x ( τ 2 ( t ) ) , x ( ξ 1 ( t ) ) , x ( ξ 2 ( t ) ) ) = q 0 ( t ) Φ γ ( x σ ( t ) ) + i = 1 2 ( 1 ) i 1 q i ( t ) Φ γ ( x ( τ i ( t ) ) ) + i = 1 2 ( 1 ) i 1 s i ( t ) Φ γ ( x ( ξ i ( t ) ) ) q 0 ( t ) Φ γ ( m 1 z σ ( t ) ) + q 1 ( t ) Φ γ ( m 1 z ( τ 1 ( t ) ) ) q 2 ( t ) Φ γ ( z ( τ 2 ( t ) ) ) + s 1 ( t ) Φ γ ( m 1 z ( ξ 1 ( t ) ) ) s 2 ( t ) Φ γ ( z ( ξ 2 ( t ) ) ) > 0 .

(ii) It is clear that [ p ( t ) z Δ ( t ) ] Δ <0 or p(t) z Δ (t) is nonincreasing since h>0 for tT. For t τ i (t)T t 0 and 1i2, we have

z σ (t)z ( τ i ( t ) ) = τ i ( t ) σ ( t ) 1 p ( s ) p(s) z Δ (s)Δsp ( τ i ( t ) ) z Δ ( τ i ( t ) ) τ i ( t ) σ ( t ) 1 p ( s ) Δs.

Dividing both sides of above inequality by z( τ i (t)), we obtain

z σ ( t ) z ( τ i ( t ) ) 1+ p ( τ i ( t ) ) z Δ ( τ i ) z ( τ i ( t ) ) P ( σ ( t ) , τ i ( t ) ) .
(2.4)

Likewise, we also have

z ( τ i ( t ) ) z(T)= T τ i ( t ) 1 p ( s ) p(s) z Δ (s)Δsp ( τ i ( t ) ) z Δ ( τ i ( t ) ) T τ i ( t ) 1 p ( s ) Δs

and

p ( τ i ( t ) ) z Δ ( τ i ( t ) ) z ( τ i ( t ) ) 1 P ( τ i ( t ) , T ) .
(2.5)

Hence, (2.4) and (2.5) imply

z σ ( t ) z ( τ i ( t ) ) 1+ p ( τ i ( t ) ) z Δ ( τ i ) z ( τ i ( t ) ) P ( σ ( t ) , τ i ( t ) ) P ( σ ( t ) , T ) P ( τ i ( t ) , T ) .

This gives the desired result

z ( τ i ( t ) ) η i (t,T) z σ (t),1i2.

For T<tσ(t) ξ j (t), 1j2, we also get

{ z ( ξ j ( t ) ) z σ ( t ) 1 + p ( σ ( t ) ) z Δ ( σ ( t ) ) z σ ( t ) P ( ξ j ( t ) , σ ( t ) ) , z σ ( t ) p ( σ ( t ) ) z Δ ( σ ( t ) ) z ( T ) p ( σ ( t ) ) z Δ ( σ ( t ) ) + P ( σ ( t ) , T ) .

Therefore, we obtain

z ( ξ j ( t ) ) z σ ( t ) 1+ p ( σ ( t ) ) z Δ ( σ ( t ) ) z σ ( t ) P ( ξ j ( t ) , σ ( t ) ) 1+ P ( ξ j ( t ) , σ ( t ) ) P ( σ ( t ) , T ) = ν j (t,T),

which yields the desired result

z ( ξ j ( t ) ) z σ (t) ν j (t,T).

(iii) It can be proved similar to [[7], Lemma 2.1] and hence its proof is omitted here. □

In addition to the above lemmas, we need a method of studying separated boundary value problems (SBVP) to prove our main results. Namely, we will define functions called upper and lower solutions that not only imply the existence of a solution of a SBVP, but that also provide bounds on the location of the solution. Consider the SBVP

where the functions fC( [ a , b ] κ 2 ×R,R), p,qC( [ a , b ] κ 2 ) with p(t)>0 and q(t)0 on [ a , b ] κ 2 . We define the set

D 1 := { y X : y Δ  is continuous and  ( p y Δ ) Δ  is rd-continuous on  [ a , b ] κ 2 } ,

where the Banach space X=C( [ a , b ] T ) is equipped with the norm defined by

y:= max t [ a , b ] T |y(t)|for all yX.

A function y is called a solution of the equation ( p ( t ) y Δ ( t ) ) Δ +q(t) y σ =0, on [ a , b ] κ 2 if y D 1 and the equation ( p ( t ) y Δ ( t ) ) Δ +q(t) y σ =0 holds for all t [ a , b ] κ 2 . Next, we define for any u,v D 1 the sector [ u , v ] 1 by

[ u , v ] 1 :={w D 1 uwv}.

Definition 2.1 [[3], Definition 6.1]

We call α D 1 a lower solution of the SBVP (2.6)-(2.7) on [ a , b ] T provided

{ ( p ( t ) α Δ ( t ) ) Δ + q ( t ) α σ ( t ) f ( t , α σ ( t ) ) for all  t [ a , b ] κ 2 , α ( a ) A , α ( b ) B .

Similarly, β D 1 is called an upper solution of the SBVP (2.6)-(2.7) on [a,b] provided

{ ( p ( t ) β Δ ( t ) ) Δ + q ( t ) β σ ( t ) f ( t , β σ ( t ) ) for all  t [ a , b ] κ 2 , β ( a ) A , β ( b ) B .

The following theorem is an extension of [[3], Theorem 6.5] to [ a , ) T .

Theorem 2.1 [[10], Theorem 1.5]

Assume that there exist a lower solution α and an upper solution β of (2.6) with α(t)β(t) for all t [ a , ) T . Then

( p ( t ) y Δ ( t ) ) Δ +q(t) y σ =f ( t , y σ )

has a solution y with y(a)=A and y [ α , β ] 1 on [ a , ) T .

We end this section with time scale version of the Arzelà-Ascoli theorem (see [[7], Lemma 2.2]) and Kranoselskii’s fixed point theorem (see [7]). These will be used in the proof of Theorem 3.3.

For T 0 , T 1 T, let [ T 0 , ) T :={tT:t T 0 } and [ T 0 , T 1 ] T :={tT: T 0 t T 1 }. Further, let C( [ T 0 , ) T ,R) denote all continuous functions mapping [ T 0 , ) T into ,

BC [ T 0 , ) T := { x : x C ( [ T 0 , ) T , R )  and  sup t [ T 0 , ) T | x ( t ) | < } .
(2.8)

Endowed on BC [ T 0 , ) T with the norm x= sup t [ T 0 , ) T |x(t)|, (BC [ T 0 , ) T ,) is a Banach space. Let XBC [ T 0 , ) T , we say X is uniformly Cauchy if for any given ε>0, there exists a T 1 [ T 0 , ) T such that for any xX,

|x( t 1 )x( t 2 )|<εfor all  t 1 , t 2 [ T 1 , ) T .

X is said to be equi-continuous on [ a , b ] T if for any given ε>0, there exists a δ>0 such that for any xX and t 1 , t 2 [ a , b ] T with | t 1 t 2 |<δ,

|x( t 1 )x( t 2 )|<ε.

Lemma 2.2 [[7], Lemma 2.2]

Suppose that XBC [ T 0 , ) T is bounded and uniformly Cauchy. Further, suppose that X is equi-continuous on [ T 0 , T 1 ] T for any T 1 [ T 0 , ) T . Then X is relatively compact.

Lemma 2.3 (Kranoselskii’s fixed point theorem)

Suppose that X is a Banach space and Ω is a bounded, convex and closed subset of X. Suppose further that there exist two operators U,S:ΩX such that

  1. (i)

    Ux+SyΩ for all x,yΩ;

  2. (ii)

    U is a contraction mapping;

  3. (iii)

    S is completely continuous.

Then U+S has a fixed point in Ω.

3 Main results

In this section, we establish our main results.

Theorem 3.1 Assume conditions (B1)-(B6) and one of (2.2)-(2.3) hold. Then any bounded solution x(t) of (1.1) is oscillatory in the case

| P(t,a)h(t, m 1 α, m 1 α η 1 ,α, m 1 α,α)Δt|=
(3.1)

for all α0 and some sufficiently large aT, where m 1 =1 r 0 , η 1 = η 1 (t,a) is given in (2.1).

Proof Assume this not to be the case and let u(t) be a bounded nonoscillatory solution of (1.1) which we may assume satisfies

u(t)>0,u ( τ i ( t ) ) >0,u ( ξ j ( t ) ) >0,tT t 0 ,1i2,1j2.

For convenience, let z 1 (t)=u(t)+r(t)u(g(t)). By Lemma 2.1, we have

z 1 Δ (t)0,u(t) ( 1 r ( t ) ) z 1 (t), z 1 ( τ 1 ( t ) ) η 1 (t,T) z 1 σ (t).

Define the function H(t, θ 1 ) as follows:

H(t, θ 1 ):=h(t, m 1 θ 1 , m 1 η 1 θ 1 , θ 1 , m 1 θ 1 , θ 1 ).
(3.2)

On one hand, by (2.2), Lemma 2.1, (B4)-(B6), the monotonicity of Φ γ (u), z 1 Δ (t)0, and η 1 = η 1 (t,T), for tT, we have

0 = [ p ( t ) z 1 Δ ( t ) ] Δ + h ( t , u σ ( t ) , u ( τ 1 ( t ) ) , u ( τ 2 ( t ) ) , u ( ξ 1 ( t ) ) , u ( ξ 2 ( t ) ) ) [ p ( t ) z 1 Δ ( t ) ] Δ + q 0 ( t ) Φ γ ( m 1 z 1 σ ( t ) ) + q 1 ( t ) Φ γ ( m 1 η 1 z 1 σ ( t ) ) q 2 ( t ) Φ γ ( z 1 σ ( t ) ) + s 1 ( t ) Φ γ ( m 1 z 1 ( ξ 1 ( t ) ) ) s 2 ( t ) Φ γ ( z 1 ( ξ 2 ( t ) ) ) [ p ( t ) z 1 Δ ( t ) ] Δ + q 0 ( t ) Φ γ ( m 1 z 1 σ ( t ) ) + q 1 ( t ) Φ γ ( m 1 η 1 z 1 σ ( t ) ) q 2 ( t ) Φ γ ( z 1 σ ( t ) ) + [ s 1 ( t ) Φ γ ( m 1 ) s 2 ( t ) ] Φ γ ( z 1 ( ξ 1 ( t ) ) ) = [ p ( t ) z 1 Δ ( t ) ] Δ + [ q 0 ( t ) Φ γ ( m 1 ) + q 1 ( t ) Φ γ ( m 1 η 1 ) q 2 ( t ) + s 1 ( t ) Φ γ ( m 1 ) s 2 ( t ) ] × Φ γ ( z 1 σ ( t ) ) = [ p ( t ) z 1 Δ ( t ) ] Δ + H ( t , z 1 σ ( t ) ) .
(3.3)

On the other hand, we can also obtain (3.3) if (2.2) is replaced by (2.3).

Applying Theorem 2.1 with α(t) z 1 (T) z 1 (t)β(t), the equation

( p ( t ) z Δ ( t ) ) Δ +H ( t , z σ ( t ) ) =0,z(T)= z 1 (T),

has a solution z(t) with z 1 (T)z(t) z 1 (t) on [ T , ) T .

It follows from Lemma 2.1 that p(t) z Δ (t) is nonincreasing and lim t p(t) z Δ (t):=L>0 exists (being finite). Integration for T<s< T implies

p ( T ) z Δ ( T ) p(s) z Δ (s)+ s T H ( u , z σ ( u ) ) Δu=0.

Letting T , we obtain

p(s) z Δ (s)=L+ s H ( u , z σ ( u ) ) Δu s H ( u , z σ ( u ) ) Δu.

It follows that

z Δ (s) 1 p ( s ) s H ( u , z σ ( u ) ) Δu.

Integrating again for T t 1 <t and by change of integration order [[11], Lemma 1]

s t [ η t f 1 ( η , ξ ) Δ ξ ] Δη= s t [ s σ ( ξ ) f 1 ( η , ξ ) Δ η ] Δξ,

we obtain

z ( t ) z ( t 1 ) t 1 t 1 p ( s ) s H ( u , z σ ( u ) ) Δ u Δ s t 1 t s t H ( u , z σ ( u ) ) p ( s ) Δ u Δ s = t 1 t t 1 σ ( u ) H ( u , z σ ( u ) ) p ( s ) Δ s Δ u t 1 t P ( u , t 1 ) H ( u , z σ ( u ) ) Δ u .

Consequently, for t t 1 T, we obtain

z(t)z( t 1 ) t 1 t P(u, t 1 )H ( u , z σ ( u ) ) Δu.

Since z(t) is bounded and t 1 t P(u,t)H(u, z σ (u))Δu is an increasing function of t, it follows that

t 1 P(u, t 1 )H ( u , z σ ( u ) ) Δu<.

Let α= z 1 σ (T); by (3.3) and Φ γ ( z 1 σ (t)) being nondecreasing, we have

P(u,T)h(u, m 1 α, m 1 η 1 α,α, m 1 α,α)Δu<.

So we obtain a contradiction to (3.1). □

Under the assumptions of Theorem 3.1, noting that (3.3), it is easy to obtain the following corollary.

Corollary 3.1 Assume conditions (B1)-(B6) and one of (2.2)-(2.3) hold. Then any bounded solution of (1.1) is oscillatory in the case

| P(t,a)h ( t , 0 , m 1 η 1 ( t , a ) α , 0 , 0 , 0 ) Δt|=

or

| P(t,a) q 1 (t) Φ γ ( m 1 η 1 ( t , a ) α ) Δt|=.

In order to extend Theorem 3.1 to unbounded solutions, we introduce the class Φ of functions ϕ such that ϕ(u) is a nondecreasing continuous function of u satisfying uϕ(u)>0, u0 with

± u 0 ± d u ϕ ( u ) <, u 0 0.
(3.4)

We say that h(t,u, v 1 , v 2 , v 3 , v 4 ) satisfies condition (C1) provided for some ϕΦ there exists c0 such that for all tT, η 1 = η 1 (t,T),

inf | u | | c | h ( t , m 1 u , m 1 η 1 u , u , m 1 u , u ) ϕ ( u ) k|h(t, m 1 c, m 1 η 1 c,c, m 1 c,c)|
(3.5)

for some positive constant k, m 1 =1 r 0 .

Theorem 3.2 Suppose ϕΦ and γ>1. Assume (B1)-(B6), and one of (2.2)-(2.3) hold. Furthermore, suppose that the function h satisfies condition (C1). If

| P(t,a)h(t, m 1 α, m 1 η 1 α,α, m 1 α,α)Δt|=
(3.6)

holds for all α0 and some sufficiently large aT, where m 1 =1 r 0 , η 1 = η 1 (t,a) is given in (2.1), then all solutions of (1.1) are oscillatory.

Proof Assume (3.6) holds for all α0 and let u(t) be an eventually positive solution of (1.1) with

u(t)>0,u ( τ i ( t ) ) >0,u ( ξ j ( t ) ) >0,tT t 0 ,1i2,1j2.

As the proof of Theorem 3.1, we have

z Δ (s) 1 p ( s ) s H ( u , z σ ( u ) ) Δu,

where H(u, z σ (u))=h(u, m 1 z σ (u), m 1 η 1 z σ (u), z σ (u), m 1 z σ (u), z σ (u)).

Let ϕ(u)= Φ γ (u), then ϕ(u)Φ. Now multiplying above inequality by [ ϕ ( z σ ( s ) ) ] 1 , we get

z Δ ( s ) ϕ ( z σ ( s ) ) 1 p ( s ) ϕ ( z σ ( s ) ) s H ( u , z σ ( u ) ) Δu= s H ( u , z σ ( u ) ) p ( s ) ϕ ( z σ ( s ) ) Δu.

We next define the continuously differentiable real-valued function

G(u):= u 0 u d s ϕ ( s ) .

Observe that G (u)=1/ϕ(u). By the Pötzsche chain rule [[2], Theorem 1.90],

( G ( z ( t ) ) ) Δ = ( 0 1 d h ϕ ( z h ( t ) ) ) z Δ (t) ( 0 1 d h ϕ ( z σ ( t ) ) ) z Δ (t)= z Δ ( t ) ϕ ( z σ ( t ) ) ,

where z h (t):=z(t)+hμ(t) z Δ (t) z σ (t).

We claim that

t 1 t z Δ ( s ) ϕ ( z σ ( s ) ) Δs t 1 t s H ( u , z σ ( u ) ) p ( s ) ϕ ( z σ ( s ) ) ΔuΔs t 1 t P(u, t 1 ) H ( u , z σ ( u ) ) ϕ ( z σ ( u ) ) Δu

for t t 1 T. By change of integration order [[11], Lemma 1], we obtain

t 1 t P ( u , t 1 ) H ( u , z σ ( u ) ) ϕ ( z σ ( u ) ) Δ u = t 1 t [ t 1 u 1 p ( s ) Δ s ] H ( u , z σ ( u ) ) ϕ ( z σ ( u ) ) Δ u t 1 t t 1 σ ( u ) 1 p ( s ) H ( u , z σ ( u ) ) ϕ ( z σ ( u ) ) Δ s Δ u = t 1 t s t H ( u , z σ ( u ) ) ϕ ( z σ ( u ) ) 1 p ( s ) Δ u Δ s t 1 t s t H ( u , z σ ( u ) ) p ( s ) ϕ ( z σ ( s ) ) Δ u Δ s .

For sufficiently large t 1 =T, by condition (C1), it immediately follows that

t 1 t z Δ ( s ) ϕ ( z σ ( s ) ) Δs t 1 t P(u, t 1 ) H ( u , z σ ( u ) ) ϕ ( z σ ( u ) ) Δuk t 1 t P(u, t 1 )H(u,c)Δu,
(3.7)

where c:=u(T)+r(T)u(g(T))>0. Since lim t u(t)=, we have

lim t G ( z ( t ) ) = lim t z ( T ) z ( t ) d u ϕ ( u ) = z ( T ) d u ϕ ( u ) <

by assumption. Therefore,

z ( T ) t ( G ( z ( s ) ) ) Δ Δs z ( T ) t z Δ ( s ) ϕ ( z σ ( s ) ) Δs z ( T ) t kP(u, t 1 ) H ( u , z σ ( u ) ) ϕ ( z σ ( u ) ) Δu.

However, letting t in above inequality, the left side is bounded whereas the right side is unbounded by assumptions (3.6), (3.7). This contradiction shows that (3.6) is sufficient for all solutions of (1.1) to be oscillatory. □

Next we will give two sufficient and necessary conditions for (1.1) being oscillatory under the case γ>1. However, we need a sufficient condition for (1.1) having a bounded nonoscillatory solution.

Theorem 3.3 Assume conditions (B1)-(B6) hold, and (2.2) or (2.3) holds. If

a P ( σ ( t ) , a ) h(t,α,α,0,α,0)Δt<
(3.8)

for some α0 and some sufficiently large aT, then (1.1) has a bounded nonoscillatory solution.

Proof Let

h 1 (t,α):=h(t,α,α,0,α,0).

Assume that (3.8) holds. Without loss of generality, we may assume α>0. Since p(t)>0 and h 1 (t,α)>0 on T, by change of integration order [[11], Lemma 1], we obtain

a s h 1 ( t , α ) p ( s ) Δ t Δ s = lim u + a u a σ ( t ) h 1 ( t , α ) p ( s ) Δ s Δ t = a a σ ( t ) h 1 ( t , α ) p ( s ) Δ s Δ t = a [ a σ ( t ) 1 p ( s ) Δ s ] h 1 ( t , α ) Δ t = a P ( σ ( t ) , a ) h 1 ( t , α ) Δ t < .
(3.9)

By (B2) and (3.9), we can choose T 0 T large enough such that

T 0 s h 1 ( t , α ) p ( s ) ΔtΔs ( 1 r 0 ) α 2 = m 1 α 2 .
(3.10)

According to (B3) and (B4), we see that there exists T 1 T with T 1 > T 0 such that g(t) T 0 and τ i (t) T 0 , 1i2, for t [ T 1 , ) T .

Define the Banach space BC [ T 0 , ) T as in (2.8), and let

Ω= { x = x ( t ) B C [ T 0 , ) T : m 1 α 2 x ( t ) α } .

It is easy to verify that Ω is a bounded, convex, and closed subset of BC [ T 0 , ) T . For the sake of convenience, set

H (t):=h ( t , x σ ( t ) , x ( τ 1 ( t ) ) , x ( τ 2 ( t ) ) , x ( ξ 1 ( t ) ) , x ( ξ 2 ( t ) ) ) .

For any xΩ and t [ T 0 , ) T , we have

0<h(t,α,α,α,α,α)< H (t)h(t,α,α, m 1 α/2,α, m 1 α/2) h 1 (t,α).
(3.11)

Now we define two operators U and S:ΩBC [ T 0 , ) T as follows:

(Ux)(t)= { r ( t ) x ( g ( t ) ) , t [ T 1 , ) T , ( U x ) ( T 1 ) , t [ T 0 , T 1 ] T

and

(Sx)(t)= { α t s H ( u ) p ( s ) Δ u Δ s , t [ T 1 , ) T , α T 1 s H ( u ) p ( s ) Δ u Δ s , t [ T 0 , T 1 ] T .

Next, we will show that U and S satisfy the conditions in Lemma 2.3.

  1. (i)

    We first prove that Ux+SyΩ for any x,yΩ. Note that for any x,yΩ, m 1 α/2x,yα. For any x,yΩ and t [ T 1 , ) T , by (3.10)-(3.11), we have

    (Ux)(t)+(Sy)(t)=αr(t)x ( g ( t ) ) t s H ( u ) p ( s ) ΔuΔs m 1 α m 1 α 2 m 1 α 2

    and

    (Ux)(t)+(Sy)(t)=αr(t)x ( g ( t ) ) t s H ( u ) p ( s ) ΔuΔsα.

    Similarly, we can show that m 1 α/2Ux+Syα for any x,yΩ and t [ T 0 , T 1 ] T .

  2. (ii)

    It is not difficult to check that U is a contraction mapping.

  3. (iii)

    We will prove that S is a completely continuous mapping. It is easy to check that S maps Ω into Ω.

Again, for the sake of convenience, let

H l (t):=h ( t , x l σ ( t ) , x l ( τ 1 ( t ) ) , x l ( τ 2 ( t ) ) , x l ( ξ 1 ( t ) ) , x l ( ξ 2 ( t ) ) ) .

Next, we show that the continuity of S. Let x l Ω and x l x0 as l, then xΩ and x l x as l. By the monotonicity and continuity of h, as l, we have

{ | H l ( t ) H ( t ) | 0 , | H l ( t ) H ( t ) | 2 h 1 ( t , α ) .

For t [ T 1 , ) T , we have

S x l S x = | S x l S x | t s | H l ( u ) H ( u ) | p ( s ) Δ u Δ s

and |(S x l )(t)(Sx)(t)|=0 for t [ T 0 , T 1 ] T . Employing Lebesgue’s dominated convergence theorem [[3], Chapter 5], we get

S x l Sx=|S x l Sx|0as l.

Thus S is continuous.

Third, we show S Ω is relatively compact. According to Lemma 2.2, it suffices to show that S Ω is bounded, uniformly Cauchy, and equi-continuous. The boundedness is obvious.

For any xΩ, by (3.10)-(3.11), we have

T 1 s H ( u ) p ( s ) ΔuΔs<.

Then for any given ε>0, there exists T 2 [ T 1 , ) T large enough such that

T 2 s H ( u ) p ( s ) ΔuΔs<ε/2.

Hence, for any xΩ and t 1 , t 2 [ T 2 , ) T , we have

( S x ) ( t 1 ) ( S x ) ( t 2 ) = | ( S x ) ( t 1 ) ( S x ) ( t 2 ) | = | t 1 s H ( u ) p ( s ) Δ u Δ s t 2 s H ( u ) p ( s ) Δ u Δ s | 2 T 2 s H ( u ) p ( s ) Δ u Δ s < 2 × ε 2 = ε .

So S Ω is uniformly Cauchy.

Finally, we will prove that S Ω is equi-continuous. For T 1 t 1 < t 2 T 2 +1, we have

( S x ) ( t 1 ) ( S x ) ( t 2 ) = | ( S x ) ( t 1 ) ( S x ) ( t 2 ) | = | t 1 s H ( u ) p ( s ) Δ u Δ s t 2 s H ( u ) p ( s ) Δ u Δ s | t 1 t 2 s H ( u ) p ( s ) Δ u Δ s .

For t 1 < T 1 t 2 T 2 +1, we have

( S x ) ( t 1 ) ( S x ) ( t 2 ) =|(Sx)( t 1 )(Sx)( t 2 )| T 1 t 2 s H ( u ) p ( s ) ΔuΔs.

For t 1 , t 2 [ T 1 , T 2 ] T , (Sx)( t 1 )(Sx)( t 2 )=0.

Therefore there exists 0<δ<1 such that |(Sx)( t 1 )(Sx)( t 2 )|<ε if t 1 , t 2 [ T 0 , T 2 +1) and | t 2 t 1 |<δ. This means that S Ω is equi-continuous.

It follows from Lemma 2.2 that S Ω is relatively compact, and then S is completely continuous.

By Lemma 2.3, there exists xΩ such that (U+S)x=x, which indicates that x(t) is a solution of (1.1). In particular, for t [ T 1 , ) T , we have

x(t)=αr(t)x ( g ( t ) ) t s H ( u ) p ( s ) ΔuΔs.

Let t, we obtain the desired result. □

Remark 3.1 Similar to the proof of Theorem 3.3, under the assumptions of Theorem 3.3, if

a P ( σ ( t ) , a ) h ( t , α , α , ( 1 r 0 ) α 2 , α , ( 1 r 0 ) α 2 ) Δt<

for some α0, then (1.1) has a bounded nonoscillatory solution.

Theorem 3.3 plays an important role in excluding (1.1) to have a unbounded nonoscillatory solution under that (3.8) holds.

Theorem 3.4 Suppose ϕΦ and γ>1. Assume (B1)-(B6) and one of (2.2)-(2.3) hold, and the function h satisfies condition (C1). Furthermore, suppose that there exists ρ 1 >0 such that

lim inf t η 1 (t,a) ρ 1 for aT
(3.12)

and

| P(t,T)h(t,0,0,α,0,α)Δt|<for all α0.
(3.13)

Then a sufficient and necessary condition for (1.1) to be oscillatory is that

| P(t,a)h(t,α,α η 1 ,0,α,0)Δt|=
(3.14)

holds for all α0 and some sufficiently large aT, where η 1 = η 1 (t,a) is given in (2.1).

Proof Assume that (3.14) holds for all α0 and let u(t)>0 be a nonoscillatory solution of (1.1). Similar to the proof of Theorem 3.2, c=u(T)+r(T)u(g(T))>0, we obtain (3.7):

t 1 t z Δ ( s ) ϕ ( z σ ( s ) ) Δs t 1 t P(u, t 1 ) H ( u , z σ ( u ) ) ϕ ( z σ ( u ) ) Δuk t 1 t P(u, t 1 )H(u,c)Δu.

By (3.12)-(3.14), for sufficiently large t t 1 T, we have

t 1 t P ( u , t 1 ) H ( u , c ) Δ u = t 1 t P ( u , t 1 ) h ( u , m 1 c , m 1 η 1 c , c , m 1 c , c ) Δ u = t 1 t P ( u , t 1 ) h ( u , m 1 c , m 1 η 1 c , 0 , m 1 c , 0 ) Δ u + t 1 t P ( u , t 1 ) h ( u , 0 , 0 , c , 0 , c ) Δ u t 1 t P ( u , t 1 ) h ( u , m 1 c , m 1 η 1 c , 0 , m 1 c , 0 ) Δ u = t 1 t P ( u , t 1 ) h ( u , α , α η 1 , 0 , α , 0 ) Δ u ,

where α= m 1 c. The rest of the proof is the same as Theorem 3.2. So we leave details to readers.

Conversely, assume that (3.12)-(3.13) hold and (3.14) does not hold for some α0, then we have

| P(t,a)h ( t , α , α η 1 ( t , a ) , 0 , α , 0 ) Δt|<.
(3.15)

Note that (3.12) implies that P(σ(t),a)/P(t,a) is bounded on T, and (3.15) holds if and only if

| P ( σ ( t ) , a ) h ( t , α , α η 1 ( t , a ) , 0 , α , 0 ) Δt|<.

According to (3.12), it follows that for any ε>0 with ε< 1 2 min ρ 1 , there exists T 1 t 0 such that η 1 (t,a) ρ 1 ε=: ρ ˆ >0 for t T 1 . It follows that |α η 1 (t,a)||α ρ ˆ | for t T 1 . Then by the monotonicity of h and the fact that η 1 (t,a)1 for t T 1 , we have

| a P ( σ ( t ) , a ) h(t,α ρ ˆ ,α ρ ˆ ,0,α ρ ˆ ,0)Δt|<,

which gives (3.8). Therefore, by Theorem 3.3, equation (1.1) has a bounded nonoscillatory solution. This contradiction shows that (3.14) is necessary. □

If (3.13) is false, (3.14) is not a necessary condition for (1.1) being oscillatory. Suppose that there exist constants β 1 >1, β 2 >1, β 3 >1 such that

q 0 (t) Φ γ ( m 1 )+ q 1 (t) Φ γ ( m 1 η 1 )> β 1 q 2 (t), s 1 (t) Φ γ ( m 1 )> β 2 s 2 (t)
(3.16)

and

q 0 (t) Φ γ ( m 1 )+ q 1 (t) Φ γ ( m 1 η 1 )+ s 1 (t) Φ γ ( m 1 )> β 3 [ q 2 ( t ) + s 2 ( t ) ] .
(3.17)

We give another sufficient and necessary condition for (1.1) to be oscillatory.

Theorem 3.5 Suppose ϕΦ and γ>1. Assume (B1)-(B6) and one of (2.2)-(2.3) hold, and the function h satisfies condition (C1). Furthermore, suppose that (3.12) and one of (3.16)-(3.17) hold. Then a sufficient and necessary condition for the second order nonlinear neutral dynamic equation (1.1) to be oscillatory is that

| P(t,a)h(t,α,α η 1 ,0,α,0)Δt|=
(3.18)

holds for all α0 and some sufficiently large aT, where η 1 = η 1 (t,a) is given in (2.1).

Since the proof of Theorem 3.5 is similar to that of Theorem 3.4, we leave the details to the readers.

For the case 0<γ1, Theorems 3.2, 3.4, and 3.5 do not hold. We introduce another class Ψ of functions ψ such that ψ(u) is a nondecreasing continuous function of u satisfying uϕ(u)>0, u0 with

± u 0 ± d u ψ ( u ) =and ± u 0 ± d u Φ γ ( u ) | ψ ( u ) | <, u 0 0.
(3.19)

Theorem 3.6 Assume 0<γ1, conditions (B1)-(B6) and one of (2.2)-(2.3) hold. Furthermore, suppose that there exists a function ψΨ which satisfies (3.19). Then any solution x(t) of (1.1) is oscillatory in the case

| [ P ( t , a ) ] γ ε h(t, m 1 α, m 1 α η 1 ,α, m 1 α,α)Δt|=
(3.20)

for all α0, some sufficiently large aT, and 0<εγ, where η 1 = η 1 (t,a) is given in (2.1).

Proof Assume not and let u(t) be a bounded nonoscillatory solution of (1.1) which we may assume satisfies

u(t)>0,u ( τ i ( t ) ) >0,u ( ξ j ( t ) ) >0,tT t 0 ,1i2,1j2.

Let

Q(t)= q 0 (t) Φ γ ( m 1 )+ q 1 (t) Φ γ ( m 1 η 1 ) q 2 (t)+ s 1 (t) Φ γ ( m 1 ) s 2 (t).

As the proof of Theorem 3.1, we also get (3.3), i.e.

[ p ( t ) z 1 Δ ( t ) ] Δ + [ ( q 0 ( t ) + q 1 ( t ) Φ γ ( η 1 ) + s 1 ( t ) ) Φ γ ( m 1 ) q 2 ( t ) s 2 ( t ) ] Φ γ ( z 1 σ ( t ) ) = [ p ( t ) z 1 Δ ( t ) ] Δ + H ( t , z 1 σ ( t ) ) = [ p ( t ) z 1 Δ ( t ) ] Δ + Q ( t ) Φ γ ( z 1 σ ( t ) ) 0 .
(3.21)

By Lemma 2.1, p(t) z 1 Δ (t)p( T 1 ) z 1 Δ ( T 1 )= c 1 >0 for t T 1 . Integrating it from T 1 to t, for t> T 2 > T 1 , we have

z 1 ( t ) z 1 ( T 1 ) + c 1 T 1 t Δ s p ( s ) [ z 1 ( T 1 ) P ( t , T 1 ) + c 1 ] P ( t , T 1 ) [ z 1 ( T 1 ) P ( T 2 , T 1 ) + c 1 ] P ( t , T 1 ) = c 2 P ( t , T 1 ) .
(3.22)

Let

ψ ( u ) = Φ 1 γ + ε ( u ) , Q 1 ( t ) = Q ( t ) / | ψ ( z 1 ( t ) / c 2 ) | , H 1 ( z 1 ( t ) ) = Φ γ ( z 1 ( t ) ) | ψ ( z 1 ( t ) / c 2 ) | , 1 > ε > 0 .

By (3.21) and (3.22), we obtain

[ p ( t ) z 1 Δ ( t ) ] Δ + Q 1 (t) H 1 ( z 1 ( t ) ) [ p ( t ) z 1 Δ ( t ) ] Δ +Q(t) Φ γ ( z 1 σ ( t ) ) 0.

Integrating the above inequality from t to T 3 , T 1 t T 3 , we have

z 1 Δ (t) 1 p ( t ) t T 3 Q 1 (s) H 1 ( z 1 ( s ) ) Δs.

Then, similar to the proof of Theorem 3.2, we have

lim T 3 T 1 T 3 z 1 Δ ( t ) Δ t H 1 ( z 1 ( t ) ) = lim T 3 z 1 ( T 1 ) z 1 ( T 3 ) Δ u H 1 ( u ) lim T 3 T 1 T 3 P ( σ ( s ) , T 1 ) Q 1 ( s ) Δ s = T 1 P ( σ ( s ) , T 1 ) Q 1 ( s ) Δ s T 1 P ( s , T 1 ) Q 1 ( s ) Δ s .

According to (3.19), we have

± u 0 ± d u H 1 ( u ) = ± u 0 ± d u Φ γ ( u ) | ψ ( u ) | <, u 0 0.

However, by (3.20) and (3.22), we have

T 1 P(s, T 1 ) Q 1 (s)Δs T 1 P ( s , T 1 ) Q ( s ) | ψ ( z 1 ( s ) / c 2 ) | Δs T 1 P ( s , T 1 ) | ψ ( P ( s , T 1 ) ) | Q(s)Δs=,

which contradicts T 1 P(s, T 1 ) Q 1 (s)Δs u 0 + d u H 1 ( u ) <. □

We will show that Theorem 3.6 is also true if ε=0 in (3.20) for 0<γ<1.

Let u,v,t,sT with u,v,t,s T 0 . Suppose that x(t)>0 be a solution of (1.1). Integrating (1.1) from v to s and dividing the resulting equation by p(s), we have

z Δ (s)=p(v) z Δ (v)/p(s) 1 p ( s ) v s hΔ θ 1 .

Again, integrating the above mentioned inequality from u to t, by Lemma 2.1 and (3.3), we have

z ( t ) = z ( u ) + p ( v ) z Δ ( v ) P ( t , u ) + u t 1 p ( s ) s v h Δ θ 1 Δ s u t 1 p ( s ) s v H ( θ 1 , z σ ( θ 1 ) ) Δ θ 1 Δ s .

Set u= T 0 and v>ts T 1 T 0 , using (3.22) and H( θ 1 ,z( θ 1 ))= H ( θ 1 , c 2 P ( θ 1 , T 0 ) ) [ c 2 P ( θ 1 , T 0 ) ] γ ( z ( θ 1 ) ) γ , we find

z ( t ) u t 1 p ( s ) s v H ( θ 1 , z σ ( θ 1 ) ) Δ θ 1 Δ s T 0 t 1 p ( s ) t v H ( θ 1 , z σ ( θ 1 ) ) Δ θ 1 Δ s P ( t , T 0 ) t v H ( θ 1 , z ( θ 1 ) ) Δ θ 1 = P ( t , T 0 ) t v H ( θ 1 , c 2 P ( θ 1 , T 0 ) ) [ c 2 P ( θ 1 , T 0 ) ] γ ( z ( θ 1 ) ) γ Δ θ 1 ,

and hence

z ( t ) P ( t , T 0 ) Z(t),where Z(t)= ( c 2 ) γ t v H ( θ 1 , c 2 P ( θ 1 , T 0 ) ) ( z ( θ 1 ) ) γ [ P ( θ 1 , T 0 ) ] γ Δ θ 1 >0.

Thus, by [[9], Lemma 2.1], we get

Z Δ ( θ 1 ) ( c 2 ) γ H ( θ 1 , c 2 P ( θ 1 , T 0 ) ) [ Z ( θ 1 ) ] γ ( 1 γ ) ( Z Δ ( θ 1 ) ) ( c 2 ) γ ( [ Z 1 γ ] Δ ( θ 1 ) ) H ( θ 1 , c 2 P ( θ 1 , T 0 ) ) ,

which implies

[ Z 1 γ ] Δ ( θ 1 ) 1 γ ( c 2 ) γ H ( θ 1 , c 2 P ( θ 1 , T 0 ) ) .

Integrating it from T 0 to t and letting t, we obtain

[ Z ( T 0 ) ] 1 γ [ Z ( t ) ] 1 γ + 1 γ ( c 2 ) γ T 0 t H ( θ 1 , c 2 P ( θ 1 , T 0 ) ) Δ θ 1 1 γ ( c 2 ) γ T 0 t H ( θ 1 , c 2 P ( θ 1 , T 0 ) ) Δ θ 1 ,

which contradicts (3.20) for ε=0.

So we have the following conclusion.

Theorem 3.7 Assume 0<γ<1, conditions (B1)-(B6) and one of (2.2)-(2.3) hold. Then any solution x(t) of (1.1) is oscillatory in the case

| [ P ( t , a ) ] γ h(t, m 1 α, m 1 α η 1 ,α, m 1 α,α)Δt|=
(3.23)

for all α0 and some sufficiently large aT, where η 1 = η 1 (t,a) is given in (2.1).

Is Theorem 3.7 also true if 0<γ<1 is replaced by γ>1? In general, it is not true. It is easy to see that (3.23) holds for γ>1, which does not imply (3.1) for all α0. Then, if (3.12)-(3.13) hold, by Theorem 3.3, all bounded solutions of (1.1) may be nonoscillatory. But it is true for unbounded solutions of (1.1).

Theorem 3.8 Assume γ>1, conditions (B1)-(B6), and one of (2.2)-(2.3) hold. Then any unbounded solution x(t) of (1.1) is oscillatory in the case

| [ P ( t , a ) ] γ h(t, m 1 α, m 1 α η 1 ,α, m 1 α,α)Δt|=
(3.24)

for all α0 and some sufficiently large aT, where η 1 = η 1 (t,a) is given in (2.1).

Proof Assume x(t)>0 be an unbounded solution of (1.1). Integrating (1.1) from T 1 to t, using t T 1 T 0 , and by (B1) and Lemma 2.1, we have

z ( t ) z ( T 1 ) = T 1 t z Δ ( s ) Δ s = T 1 t p ( s ) z Δ ( s ) p ( s ) Δ s P ( t , T 1 ) [ p ( t ) z Δ ( t ) ] T 1 t P ( t , T 1 ) [ p ( s ) z Δ ( s ) ] Δ Δ s ,

which implies that

z(t)>P(t, T 1 ) [ p ( t ) z Δ ( t ) ] ,t T 1 T 0 .

By (3.3) and z Δ (t)>0 for t T 0 , we get

H ( t , z σ ( t ) ) H ( t , z ( t ) ) >H ( t , P ( t , T 1 ) [ p ( t ) z Δ ( t ) ] ) =Q(t) Φ γ ( P ( t , T 1 ) [ p ( t ) z Δ ( t ) ] ) >0.

Let y(t)=p(t) z Δ (t), then

y Δ (t)H ( t , z σ ( t ) ) >Q(t) Φ γ ( P ( t , T 1 ) y ( t ) ) >0.

Both sides divide Φ γ (y(t)); integrating it from T 2 to T 3 , T 3 > T 2 T 1 , and noting that 0y(t)<y( T 0 ), t T 0 , we have

0 < T 2 T 3 Q ( t ) Φ γ ( P ( t , T 1 ) ) Δ t < T 2 T 3 y Δ ( t ) Φ γ ( y ( t ) ) Δ t = y ( T 3 ) y ( T 2 ) 1 Φ γ ( u ) Δ u 0 y ( T 2 ) 1 Φ γ ( u ) Δ u = .

Letting T 3 and a= T 1 , we obtain

0< T 2 Q(t) Φ γ ( P ( t , T 1 ) ) Δt= T 2 [ P ( t , T 1 ) ] γ h(t, m 1 α, m 1 η 1 α,α, m 1 α,α)Δt<,

which contradicts (3.24). The proof is complete. □

4 Examples

We would like to illustrate the results by means of the following examples.

Example 4.1 Let Φ (u)= | u | 1 u, nN, σ n (t)=σ( σ n 1 (t)), ρ n (t)= ρ n 1 (t), h>0 is a constant, time scale T=hZ. Consider the dynamic equation

[ p ( t ) ( x ( t ) + r 0 x ( g ( t ) ) ) Δ ] Δ +h ( σ ( t ) , x ( τ 1 ( t ) ) , x ( τ 2 ( t ) ) , x ( ξ 1 ( t ) ) , x ( ξ 2 ( t ) ) ) =0,
(4.1)

where g(t)=ρ(t), 0 r 0 <1 is a constant. τ 1 (t)=ρ(t), τ 2 (t)=t, ξ 1 (t)= σ 3 (t), ξ 2 (t)= σ 2 (t), q 0 (t)=t, q 1 (t)= t , q 2 (t)=lnt, s 1 (t)=1, s 2 (t)= t 2 . We assume that p(t)>0 is nondecreasing and satisfies (B1). For sufficiently large tT, it is not difficult to check that conditions (B2)-(B6), (2.2), and (3.17) hold. By Lemma 2.1, for sufficiently large tT, we have

η 1 τ 1 (t)/σ(t)=(th)/(t+h)1andP(t,a)= a t Δ s p ( s ) 1,taT

and

| q 1 (t) Φ γ ( m 1 η 1 α)Δt|=| q 1 (t) Φ γ ( m 1 α)Δt|=.
(4.2)

According to Corollary 3.1, any bounded solution of (4.1) is oscillatory.

Let ϕ(u)= Φ γ (u) and γ>1, we obtain

inf | u | | c | h ( t , m 1 u , m 1 η 1 u , u , m 1 u , u ) ϕ ( u ) k|h(t, m 1 c, m 1 η 1 c,c, m 1 c,c)|

for some positive constant k and k| Φ γ (c)|1. Condition (C1) is satisfied. Since η 1 1, (3.12) holds. Equations (4.2) and (3.17) imply (3.18) holds, so we give a sufficient and necessary condition for all solutions of (4.1) being oscillatory.

Let ψ(u)= Φ 1 γ + ε (u), 0<εγ<1, then (3.19) holds. Hence, by Theorem 3.6, all solutions of (1.1) are oscillatory because (4.2) and (3.17) imply (3.20).

In particular, (4.1) becomes the classical difference equation if h=1.

Remark 4.1 Let T= q N , q>1 be a constant; T= N 0 2 ={ n 2 :n N 0 }; T={ H n :n N 0 }, where H n are the so-called harmonic numbers, H 0 =0, H n = k = 1 n 1 k for nN. Then the conclusion of Example 4.1 is also true under the same assumptions.

Example 4.2 Let Φ (u)= | u | 1 u, the time scale T= P a , b = k = 0 [k(a+b),k(a+b)+a], a>0, b0 are constants. Consider the dynamic equation

[ t 3 ( x ( t ) + ( 1 / 4 e t ) x ( g ( t ) ) ) Δ ] Δ + Φ γ ( x σ ( t ) ) + Φ γ ( x ( τ 1 ( t ) ) ) 2 γ Φ γ ( x ( τ 2 ( t ) ) ) = 0 ,
(4.3)

where m 1 =1(1/4 e t )3/4. We assume that g(t) is rd-continuous on [ t , ) T which satisfies (B2). For k 1 , k 2 N, and k 1 k 2 , τ 1 (t), τ 2 (t) are defined as follows:

τ 1 (t)= { 0 if  t k = 0 k 1 [ k ( a + b ) , k ( a + b ) + a ] , t k 1 ( a + b ) if  t k = k 1 [ k ( a + b ) , k ( a + b ) + a ]

and

τ 2 (t)= { 0 if  t k = 0 k 2 [ k ( a + b ) , k ( a + b ) + a ] , t k 2 ( a + b ) if  t k = k 2 [ k ( a + b ) , k ( a + b ) + a ] .

Then σ(t)=t, t[k(a+b),k(a+b)+a), σ(t)=t+b, t=k(a+b)+a, kN. It is easy to check that conditions (B1)-(B6) and (2.2) hold,

| Φ γ (3/4α)+ Φ γ (3/4 η 1 α) 2 γ Φ γ (α)Δt|=.

According to Corollary 3.1, any bounded solution of (4.3) is oscillatory.

Similar to Example 4.1, for any γ>0, it is easy to check that condition (C1) (γ>1) and (3.19)-(3.20) (0<γ1) hold, respectively. Then we see that (4.3) is oscillatory.

In particular, (4.3) becomes the classical differential equations if b=0.

Example 4.3 Let Φ (u)= | u | 1 u and time scale T=R. Consider the differential equation

( x ( t ) + r 0 x ( g ( t ) ) ) + q 0 Φ 2 ( x ( t ) ) + q 1 Φ 2 ( x ( τ 1 ( t ) ) ) q 2 Φ 2 ( x ( τ 2 ( t ) ) ) + s 1 Φ 2 ( x ( ξ 1 ( t ) ) ) s 2 Φ 2 ( x ( ξ 2 ( t ) ) ) = 0 ,
(4.4)

where r 0 =1/3, m 1 =1 r 0 =2/3, g(t)=tlnt, τ 1 (t)=t12, τ 2 (t)=t1sint/4, ξ 1 (t)=2t, ξ 2 (t)=t+3, q 0 =10, q 1 =8, q 2 =7, s 1 =36, s 2 =5. It is not difficult to check that conditions (B1)-(B6) hold. Since s 1 Φ 2 ( m 1 ) q 2 s 2 =4>0, it is easy to see that (2.3) and (3.17) hold. Similar to Example 4.1, we see that the function

h ( t , x 0 , x 1 , x 2 , x 3 , x 4 ) = q 0 Φ 2 ( x ( t ) ) + q 1 Φ 2 ( x ( τ 1 ( t ) ) ) q 2 Φ 2 ( x ( τ 2 ( t ) ) ) + s 1 Φ 2 ( x ( ξ 1 ( t ) ) ) s 2 Φ 2 ( x ( ξ 2 ( t ) ) )

satisfies condition (C1). Finally, we show that (3.12) holds. By Lemma 2.1(iii),

η 1 = η 1 (t,T)= τ 1 ( t ) τ 1 ( T ) t T τ 1 ( t ) t = t ln t t 1,tT,

so (3.12) holds. For any α0,

| P ( t , a ) h ( t , α , α η 1 , 0 , α , 0 ) d t | = | ( t a ) [ 10 Φ 2 ( α ) + 8 Φ 2 ( α ) + 36 Φ 2 ( α ) ] d t | = .

By Theorem 3.5, (4.4) is oscillatory.

References

  1. 1.

    Agarwal RP, Grace SR, O’Regan D Series in Mathematical Analysis and Applications 5. In Oscillation Theory for Second Order Dynamic Equations. Taylor & Francis, London; 2003.

    Google Scholar 

  2. 2.

    Bohner M, Peterson A: Dynamic Equations on Time Scales: An Introduction with Applications. Birkhäuser, Boston; 2001.

    Google Scholar 

  3. 3.

    Bohner M, Peterson A (Eds): Advances in Dynamic Equations on Time Scales. Birkhäuser, Boston; 2003.

    Google Scholar 

  4. 4.

    Saker SH: Oscillation Theory of Dynamic Equations on Time Scales: Second and Third Orders. Lambert Academic Publishing, Saarbrücken; 2010.

    Google Scholar 

  5. 5.

    Agarwal RP, Bohner M, O’Regan D, Peterson A: Dynamic equations on time scales: a survey. J. Comput. Appl. Math. 2002, 141: 1–26. 10.1016/S0377-0427(01)00432-0

    MathSciNet  Article  MATH  Google Scholar 

  6. 6.

    Agarwal RP, Bohner M, Řehák P: Half-linear dynamic equations. 1. In Nonlinear Analysis and Applications: to V. Lakshmikantham on His 80th Birthday. Kluwer Academic, Dordrecht; 2003:1–57.

    Google Scholar 

  7. 7.

    Deng XH, Wang QR: Oscillation and nonoscillation for second-order nonlinear neutral functional dynamic equations on time scales. Electron. J. Differ. Equ. 2013., 2013: Article ID 234

    Google Scholar 

  8. 8.

    El-Morshedy HA: New oscillation criteria for second order linear difference equations with positive and negative coefficients. Comput. Math. Appl. 2009, 58: 1988–1997. 10.1016/j.camwa.2009.07.078

    MathSciNet  Article  MATH  Google Scholar 

  9. 9.

    Grace SR, Agarwal RP, Bohner M, O’Regan D: Oscillation of second-order strongly superlinear and strongly sublinear dynamic equations. Commun. Nonlinear Sci. Numer. Simul. 2009, 14: 3463–3471. 10.1016/j.cnsns.2009.01.003

    MathSciNet  Article  MATH  Google Scholar 

  10. 10.

    Higgins R: Some oscillation results for second order functional dynamic equations. Adv. Dyn. Syst. Appl. 2010, 5: 87–105.

    MathSciNet  Google Scholar 

  11. 11.

    Karpuz B: Unbounded oscillation of higher-order nonlinear delay dynamic equations of neutral type with oscillating coefficients. Electron. J. Qual. Theory Differ. Equ. 2009., 2009: Article ID 34

    Google Scholar 

  12. 12.

    Manojlovic J, Shoukaku Y, Tanigawa T, Yoshida N: Oscillation criteria for second order differential equations with positive and negative coefficients. Appl. Math. Comput. 2006, 181: 853–863. 10.1016/j.amc.2006.02.015

    MathSciNet  Article  MATH  Google Scholar 

  13. 13.

    Özbekler, A, Zafer, A: Second order oscillation of mixed nonlinear dynamic equations with several positive and negative coefficients. Discrete Contin. Dyn. Syst., Dynamical systems, differential equations and applications. 8th AIMS Conference. Suppl. Vol. II, 1167–1175 (2011). ISBN:978–1-60133–008–6; ISBN:1–60133–008–1

  14. 14.

    Özbekler A, Wong JSW, Zafer A: Forced oscillation of second order nonlinear differential equations with positive and negative coefficients. Appl. Math. Lett. 2011, 24: 1125–1130.

    Article  MathSciNet  MATH  Google Scholar 

  15. 15.

    Tang XH, Yu JS, Peng DH: Oscillation and nonoscillation of neutral difference equations with several positive and negative coefficients. Comput. Math. Appl. 2000, 39(7–8):169–181. 10.1016/S0898-1221(00)00073-0

    MathSciNet  Article  MATH  Google Scholar 

  16. 16.

    Thandapani E, Muthulakshmi V, Graef JR: Oscillation criteria for second order nonlinear neutral delay differential equations with positive and negative coefficients. Int. J. Pure Appl. Math. 2011, 70: 261–274.

    MathSciNet  MATH  Google Scholar 

  17. 17.

    Weng A, Sun J: Oscillation of second order delay differential equations. Appl. Math. Comput. 2008, 198: 930–935. 10.1016/j.amc.2007.09.016

    MathSciNet  Article  MATH  Google Scholar 

  18. 18.

    Bai Y, Liu L: New oscillation criteria for second-order neutral delay differential equations with positive and negative coefficients. Abstr. Appl. Anal. 2010., 2010: Article ID 564068

    Google Scholar 

Download references

Acknowledgements

The authors would like to express their great gratitude to the anonymous valuable suggestions and comments, which helped the authors to improve the previous version of this article. This work was supported by the NNSF of P.R. China (Grant No. 11271379).

Author information

Affiliations

Authors

Corresponding author

Correspondence to Ravi P Agarwal.

Additional information

Competing interests

The authors declare that they have no competing interests.

Authors’ contributions

The first author discovered the topic, offered the main ideas for the proof of the paper, and carried out writing this article. The first and the second authors discussed the paper together, and all the authors interchanged ideas about this paper. The second and the third authors gave some helpful suggestions for writing the paper and checked the proof of the paper. All authors read and approved the final manuscript.

Rights and permissions

Reprints and Permissions

About this article

Verify currency and authenticity via CrossMark

Cite this article

Deng, X., Wang, Q. & Agarwal, R.P. Oscillation and nonoscillation for second order neutral dynamic equations with positive and negative coefficients on time scales. Adv Differ Equ 2014, 115 (2014). https://doi.org/10.1186/1687-1847-2014-115

Download citation

Keywords

  • neutral dynamic equations
  • positive and negative coefficients
  • oscillation and nonoscillation
  • lower and upper solutions
  • Kranoselskii’s fixed point theorem