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Selçuk J. Appl. Math. Selçuk Journal of Vol. 11. No. 2. pp. 55-62, 2010 Applied Mathematics

Oscillation Results of Higher Order Nonlinear Neutral Delay Differ-ential Equations

M. K. Yıldız, Ö. Öcalan

Afyon Kocatepe University, Faculty of Science and Arts, Department of Mathematics, ANS Campus, 03200, Afyon, Türkiye

e-mail: myildiz@ aku.edu.tr,ozkan@aku.edu.tr

Received Date: November 2, 2009 Accepted Date: August 11, 2010

Abstract. In this paper, we shall consider higher order nonlinear neutral delay differential equation of the type

[() + ()( ())]()+ ()[(())]= 0  ≥ 0  ∈ N

where   ∈ ([0 ∞) [0 ∞))    ∈ ([0 ∞) R) ()   lim→∞ () = ∞

()   lim→∞() = ∞ and  ∈ (0 ∞) is a ratio of odd positive integers.

We obtain sufficient conditions for the oscillations of all solutions of this equa-tion.

Key words: Oscillation, differential equation, neutral, delay, nonlinear. 2000 Mathematics Subject Classification. 34C10,34K15, 34K40, 35B05, 35L20. 1. Introduction

We consider the following higher order nonlinear neutral delay differential equa-tion:

(1.1) [() + ()( ())]()+ ()[(())]= 0  ≥ 0  ∈ N

where   ∈ ([0 ∞) [0 ∞))    ∈ ([0 ∞) R) ()   lim→∞ () = ∞

()   lim→∞() = ∞ and  ∈ (0 ∞) is a ratio of odd positive integers. If

0    1 equation (11) is called sublinear equation, when   1 it is called superlinear equation.

Recently, there have been a lot of studies concerning the behaviour of the oscil-latory differential equations, see [1-9] and the reference cited therein. In [2,4,6,8] several authors have investigated the following first order nonlinear delay dif-ferential equation of the form,

(1.2) 0() + ()[(())]= 0  ≥  0

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where  ∈ ([0 ∞) [0 ∞))  ∈ ([0 ∞) R) ()   lim→∞() = ∞ and

 ∈ (0 ∞) is a ratio of odd positive integers.

When 0    1 it is shown that every solution of sublinear equation (12) oscillates if and only if

(1.3)

Z

=0

() = ∞

When  = 1 (12) reduces to the linear delay differential equation (1.4) 0() + ()(()) = 0  ≥ 0

Recently, the oscillatory behavior of (14) has been discussed extensively in the literature. A classical result is (see[2,4]) that every solution of (14) oscillates if

lim inf →∞  Z () ()  1 

In [6], when   1 Tang obtained the oscillatory behavior of equation (12) It is shown that, let () is continuously differentiable and 0() ≥ 0 Further,

suppose that there exist a continuously differentiable function () such that 0()  0 and lim →∞() = ∞ lim sup →∞ ∙0(())0() 0() ¸  1 and lim inf →∞ ∙ ()−() 0() ¸  0

Then every solution of superlinear equation (12) oscillates. Furthermore, Tang considered the following special form of (12)

(1.5) 0() + ()[( − )]= 0  ≥ 0

which was obtained, if exists   −1ln  such that

(1.6) lim inf

→∞ [() exp(

−)]  0

then every solution of (15) oscillates.

In [1] Agarwal and Grace, in [3] Grace and Lalli studied oscillatory behavior of certain higher order differential equations.

Our aim in this paper is to obtain sufficient conditions for the oscillation of all solutions of (11).

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Lemma 1.1. (See[8].)Assume that for large  () 6= 0 for  ∈ [ ∗] where ∗ satisfies () =  Then

0() + ()[(())]= 0  ≥ 0

has an eventually positive solution if and only if the corresponding inequality 0() + ()[(())]≤ 0  ≥ 0

has an eventually positive solution.

Lemma 1.2. (See[5].)Let  be a positive and -times diferentiable function on [0 ∞). If  is of constant sign for  ≥  and not identically zero on any

interval [ ∞) for some ≥ 0, then, there exists a ≥ 0 and an integer ,

0 ≤  ≤  with ( + ) odd for ()() ≤ 0, or ( + ) even for ()() ≥ 0,

and such that for every ≥ 0,

 ≤  − 1 implies (−1)+()()  0,  =   + 1 · · ·   − 1, and

  0 implies ()()  0  = 0 1 · · ·   − 1

Lemma 1.3. (See[7].)Let  be as in Lemma 1.2. In addition lim→∞() 6= 0

and (−1)()()() ≤ 0 for every  ≥ 

 then for every  0    1 the

following hold:

() ≥  ( − 1)!

−1(−1)(); for all large 

2. Sufficient Conditions for Oscillations of Equation (1.1)

Theorem 2.1. (a) Let  be even and 0 ≤ ()  1 for  ≥ 0. If the diferential

equation (2.1) 0() + ()[(())]= 0 where (2.2) () = () µ ( − 1)! ¶ [1 − (())](())(−1) is oscillatory, then all solutions of (11) are oscillatory.

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(b) Let  be odd and 0 ≤ () ≤ 1  1 where 1 is a constant. If the diferential equation (2.3) 0() + ()[(())]= 0 where (2.4) () = ()2 µ  ( − 1)! ¶ (())(−1)[(())]

is oscillatory, then every solution of (11) either oscillates or tends to zero as  → ∞.

Proof. Let () be a nonoscillatory solution of (11), with ()  0, ( ())  0 and (())  0, for all  ≥ 0≥ 0. Setting () = () + ()( ()), we get

() ≥ ()  0 and

(2.5) ()() = −()(())  0

for  ≥ 0. Then by Lemma 12, ()() is of constant sign for  = 1 2 3  ,

and that for  ≥ 2

(2.6) (−1)()  0   ≥ 0

We claim that 0() ≤ 0 eventually. This is obvious from equation (11) in the

case  = 1. For  ≥ 2, we suppose on the contrary, that 0()  0 for  ≥ 1≥ 0.

Then

(2.7) (1 − ())() ≤ () − ()(()) = () − ()( ())((())) ≤ () for  ≥ 2≥ 1. Since () is positive and increasing, it follows from Lemma 13

and (27), that

(2.8) () ≥

( − 1)!

−1(−1)()  ≥  2

Using (28), we find for  ≥ 2≥ 1,

()(()) ≥ ()[1 − (())] ( − 1)! (()) −1(−1)(()) and so ()() ≤ −() µ [1 − (())] ( − 1)! ¶ (())(−1)h(−1)(())i  .

Using the above inequality in (25), we see that (−1)() is an eventually positive

(see (26)) solution of ()() + () µ [1 − (())] ( − 1)! ¶ (())(−1)h(−1)(())i≤ 0

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If we chose (−1)() = (), then 0() + () µ  ( − 1)! ¶ [1 − (())](())(−1)(()) ≤ 0 for some 3≥ 2 and hence by (26) we have

0() + ()[(())]≤ 0 for  ≥ 3

Therefore by Lemma 11, (21) has eventually positive solution, this is a contra-diction. Hence, 0() ≤ 0 eventually.

Since 0() ≤ 0 eventually in Lemma 12, we must have  = 0 and

(2.9) (−1)()()  0 0 ≤  ≤  − 1  ≥ 0

If  is even, (29) yields to contradiction (26). This proves part () of the theorem.

Now, let  be odd. Assume further that () does not tend to zero as  → ∞ As 0() ≤ 0 eventually, we have () ↓  as  → ∞ where 0    ∞ Then,

there exists   0 and an integer 3 0 such that

0    1 − 1 1 + 1

  and

(2.10)  −   () ≤ ( ())   +   ≥ 3

Thus, from (27) and (210) we find for  ≥ 3

(2.11) () ≥ ()−()(()) ≥ ()−1( ())  (−)−1(+)  1()

where 1= [( − ) − 1( + )]( + ) ∈ (0 1) Using (211) and Lemma 13,

we get for  ≥ 4≥ 3 (2.12) ()  1()  1(−1)! −1(−1)() By (212) we obtain for  ≥ 5≥ 4 ()(()) ≥ ()1  ( − 1)!(()) −1(−1)(()) There, we have ()() + ()(1) µ  ( − 1)! ¶ (())(−1)h(−1)(())i≤ 0 Using the above inequality in (25), we see that (−1)() is an eventually positive (see (26)) solution of 0() + ()2 µ  ( − 1)! ¶ (())(−1)(()) ≤ 0

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where () = (−1)() and 2 = (1) Therefore by Lemma 11, (21) has

eventually positive solution, this is a contradiction. The proof of part () is complete.

Theorem 2.2. Let −1  −2 ≤ () ≤ 0 where 2  0 is a constant. If the

differential equation (2.13) 0() + ()[(())]= 0 where (2.14) () = () µ  ( − 1)! ¶ (())(−1)[(())]

is oscillatory, then each monotone solution of (11) tends to zero as  → ∞. Proof. Let () be a monotone solution of (11). The case  = 1 can be proved easily. Assume that  ≥ 2 and ()  0, (())  0 and (())  0, for all  ≥ 0 ≥ 0 Furter, we assume that () does not tend to zero as  → ∞

Setting () = () + ()( ()), we get () ≤ () and also inequality (25). Since  is monotone, we have either 0() ≤ 0 or 0()  0 eventually.

We claim that 0() ≤ 0 eventually. This is obvious from equation (11) in the

case  = 1. For  ≥ 2, we suppose on the contrary, that 0()  0 for  ≥ 1≥ 0.

Since −1  −2≤ () ≤ 0 we get for  ≥ 2≥ 1,

(2.15) () ≥ () + ()() ≥ (1 − 2)()  0

Thus, 0() is of one sign, i.e., either 0() ≤ 0 or 0()  0 holds for  ≥ 3≥ 2

by Lemma 12.

(i) Assume that 0() ≤ 0 Then () converges to a constant 1≥ 0 If 1= 0

by (215) () converges to 0, this contradicts to 0() ≥ 0 ()  0 Hence,

1 0 Given 1∈ (0 1), there exists 4≥ 3 such that

(2.16) 1− 1  ()  1+ 1  ≥ 4

Let m be as in Lemma 13 For  ≥ 5 ≥ 2−14 using (216) and Lemma 13

successively, we obtain (2.17) () ≥ () ≥  ( − 1)! −1(−1)()  ≥  5 By (217), we obtain for  ≥ 6≥ 5 ()() ≤ −() µ  ( − 1)! ¶ (())(−1)h(−1)(())i If we chose (−1)() = (), then 0() + () µ  ( − 1)! ¶ (())(−1)[(())]≤ 0

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Using the above inequality in (25), we see that (−1)() is an eventually positive (see (26)) solution of (2.18) 0() + () µ  ( − 1)! ¶ (())(−1)[(())]≤ 0

Therefore by Lemma 11, (213) has eventually positive solution, this is a con-tradiction.

(ii) Assume that 0()  0  ≥ 7 Then by Lemma 13 we have for  ≥ 7

() ≥  ( − 1)!

−1(−1)()  ≥  7

and the inequality ()() + () µ  ( − 1)! ¶ (())(−1)h(−1)(())i≤ 0

where (−1)() = (), has an eventually positive solution This is a

contradic-tion.

Consequently, 0() ≤ 0 eventually, which tells us that () is nonincreasing and

bounded from below, and so coverges to a constant 0≥ 0 If 0= 0 then the

result is true. Assume that 0 0 Then we have

(2.19) lim inf

→∞ () = (1 + lim inf→∞ ())0≥ (1 − 2)0 0

Hence, () is eventualy positive and (26) holds. By Lemma 12, either 0()  0

or 0()  0 holds for  ≥ 8 Similar to the above proof of (i) and (ii)  we can also

obtain contradiction. The case when () is monotone and eventualy negative can be verified similarly. The proof is complete.

References

1. R. P. Agarwal and S. R. Grace, Oscillation of Certain Functional Differential Equations, Computers & Math. Applic. 38, 143-153, (1999).

2. L. H. Erbe, Q. Kong and B. G. Zhang, Oscillation Theory for Functional Differential Equations, Marcel Dekker, New York, 1995.

3. S. R. Grace and B. S. Lalli, Oscillation Theorems forOrder Delay Differential

Equations, J. Math. Anal. Appl. 91, 352-366, (1983).

4. I. Gyori and G. Ladas, Oscillation Theory of Delay Differential Equations with Applications, Clarendon Press, Oxford, 1991.

5. I. T. Kiguratze, On oscillatory solutions of some ordinary differential equations, Soviet Math. Dokl.144, 33-36, (1962).

6. G. S. Ladde, V. Lakshmıkantham and B. G. Zhang, Oscillation theory of differential equations with deviating arguments, Macel Dekker, New York, 1987.

7. W. T. Li and S. S. Cheng, An Oscillation Theorem for Higher Order Nonhomoge-neous Superlinear Differential Equations, Appl. Math. E-Notes, 3, 58-65, (2003).

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8. X. H. Tang, Oscillation for first order superlinear delay differential equations, J. London Math. Soc. (2) 65, 115-122 (2002).

9. M. K. Yildiz, Oscillation Results of Higher Order Nonlinear Neutral Delay Differ-ential Equations With Oscillating Coefficients, Adv. Dynam. Syst. Appl. (ADSA), (accepted), (2008).

Referanslar

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