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Oscillation of Second-Order Sublinear Dynamic Equations with Damping on Isolated Time Scales
Advances in Difference Equations volume 2010, Article number: 103065 (2010)
Abstract
This paper concerns the oscillation of solutions to the second sublinear dynamic equation with damping , on an isolated time scale which is unbounded above. In , α is the quotient of odd positive integers. As an application, we get the difference equation , where , , and is any real number, is oscillatory.
1. Introduction
During the past years, there has been an increasing interest in studying the oscillation of solution of second-order damped dynamic equations on time scale which attempts to harmonize the oscillation theory for continuousness and discreteness, to include them in one comprehensive theory, and to eliminate obscurity from both. We refer the readers to the papers [1–4] and the references cited therein.
In [5], Bohner et al. consider the second-order nonlinear dynamic equation with damping
where and are real-valued, right-dense continuous functions on a time scale , with . is continuously differentiable and satisfies and for . When , where , is the quotient of odd positive integers, (1.1) is the second-order sublinear dynamic equation with damping
When , (1.2) is the second-order sublinear dynamic equation
When , (1.3) is the second-order sublinear difference equation
In [6], under the assumption of being an isolated time scale, we prove that, when is allowed to take on negative values, is sufficient for the oscillation of the dynamic equation (1.3). As an application, we get that, when is allowed to take on negative values, is sufficient for the oscillation of the dynamic equation (1.4), which improves a result of Hooker and Patula [7, Theorem 4.1] and Mingarelli [8].
In this paper, we extend the result of [6] to dynamic equation (1.1). As an application, we get that the difference equation with damping
where , , , and is any real number, is oscillatory.
For completeness (see [9, 10] for elementary results for the time scale calculus), we recall some basic results for dynamic equations and the calculus on time scales. Let be a time scale (i.e., a closed nonempty subset of ) with . The forward jump operator is defined by
and the backward jump operator is defined by
where , where denotes the empty set. If , we say is right scattered, while, if , we say is left scattered. If , we say is right dense, while, if and , we say is left-dense. Given a time scale interval in the notation denotes the interval in case and denotes the interval in case . The graininess function μ for a time scale is defined by , and for any function the notation denotes . We say that is differentiable at provided
exists when (here, by , it is understood that approaches in the time scale) and when is continuous at and
Note that if , then the delta derivative is just the standard derivative, and when the delta derivative is just the forward difference operator. Hence, our results contain the discrete and continuous cases as special cases and generalize these results to arbitrary time scales (e.g., the time scale which is very important in quantum theory [11]).
2. Lemmas
We will need the following second mean value theorem (see [10, Theorem 5.45]).
Lemma 2.1.
Let be a bounded function that is integrable on . Let and be the infimum and supremum, respectively, of the function on . Suppose that is nonincreasing with on . Then, there is some number with such that
Lemmas 2.2 and 2.4 give two lower bounds of definite integrals on time scale, respectively.
Lemma 2.2.
Assume that , where . If there exists a real number such that , for all , then, for , , one has
Remark 2.3.
It is easy to know that, when , and, when , .
Proof.
For , using Theorem 1.75 of [9], we have
We consider the two cases and . First, if , then we have that
On the other hand, if , then
which implies that
From (2.3)–(2.6) and the additivity of the integral, we have
Lemma 2.4.
Assume that , where , with . Then, for , , one has
Proof.
For , using Theorem 1.75 of [9], we have
Setting , we have that
We consider the two possible cases and . First, if , we have that
On the other hand, if , then
which implies that
Hence, from (2.10)–(2.13), we have that
From (2.9), (2.10), (2.14), and the additivity of the integral, we have
3. Main Theorem
Theorem 3.1.
Assume that , where . Suppose that
(i)there exists a real number such that , for all ;
(ii)there exists a function such that for ,
Then, (1.1) is oscillatory.
Proof.
For the sake of contradiction, assume that (1.1) is nonoscillatory. Then, without loss of generality, there is a solution of (1.1) and a with , for all . Making the substitution in (1.1) and noticing that
we get that
Multiplying both sides of (3.3) by , integrating from to , and using an integration by parts formula, we get
Next, using the quotient rule and then Pötzsche's chain rule [9, Theorem 1.90] gives
where we used the fact that . Using this last inequality in (3.4), we get
Note that
Let us define , . Then, we get from (3.6) and (3.7) that
since , for . So the first term of (3.8) is nonnegative. From (3.8), we get that
From and , using the second mean value theorem [10, Theorem 5.45] and Lemmas 2.2 and 2.4, we get that
From and , the fifth term of (3.9) is nonnegative. From (3.9), and (3.10), we get that
Since , from (3.11), there exists such that, for , we have
Dividing both sides of this last inequality by and integrating from to , we get, using inequality (2.11) in [12], that
Since , we get , for large , which is a contradiction. Thus, (1.1) is oscillatory.
When , , and , it is easy to get that , . So we have the following corollary (see Corollary 2.4 of [6]). Corollary 3.2 shows that, with no sign assumption on , the condition
is sufficient for the oscillation of the difference equation (1.4).
Corollary 3.2.
Assume that . If
then (1.4) is oscillatory.
By using the idea in Theorem 3.1, we can also consider the differential equation
where . It is easy to get the following.
Theorem 3.3.
Suppose that there exists a function such that
Then, the differential equation (3.16) is oscillatory.
Example 3.4.
Consider the sublinear difference equation
where , , , and is any real number.
Take , . We have
Let . Then, we have , for large . So is concave for large . Therefore, we have
for large . That means . It is easy to get that and is nonincreasing for large . So from Theorem 3.1, (3.18) is oscillatory.
Example 3.5.
Let , , and consider the -difference equation
where , , , is any real number. Take . We have
and is nonincreasing. So from Theorem 3.1, (3.21) is oscillatory.
Example 3.6.
Let , and consider the differential equation
where , , , and is any real number.
Take . It is easy to know that
So from Theorem 3.3, (3.23) is oscillatory.
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Acknowledgment
This work was supported by the National Natural Science Foundation of China (no. 10971232).
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Lin, Q., Jia, B. Oscillation of Second-Order Sublinear Dynamic Equations with Damping on Isolated Time Scales. Adv Differ Equ 2010, 103065 (2010). https://doi.org/10.1155/2010/103065
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DOI: https://doi.org/10.1155/2010/103065