Volume 2011, Issue 1 754350
Research Article
Open Access

Explicit Bounds to Some New Gronwall-Bellman-Type Delay Integral Inequalities in Two Independent Variables on Time Scales

Fanwei Meng

Corresponding Author

Fanwei Meng

School of Mathematical Sciences, Qufu Normal University, Qufu 273165, China qfnu.edu.cn

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Qinghua Feng

Qinghua Feng

School of Mathematical Sciences, Qufu Normal University, Qufu 273165, China qfnu.edu.cn

School of Science, Shandong University of Technology, Zibo 255049, China sdut.edu.cn

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Bin Zheng

Bin Zheng

School of Science, Shandong University of Technology, Zibo 255049, China sdut.edu.cn

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First published: 13 October 2011
Citations: 5
Academic Editor: Bernard Geurts

Abstract

Some new Gronwall-Bellman-type delay integral inequalities in two independent variables on time scales are established, which provide a handy tool in the research of qualitative and quantitative properties of solutions of delay dynamic equations on time scales. The established inequalities generalize some of the results in the work of Zhang and Meng 2008, Pachpatte 2002, and Ma 2010.

1. Introduction

During the past decades, with the development of the theory of differential and integral equations, a lot of integral and difference inequalities have been discovered, which play an important role in the research of boundedness, global existence, stability of solutions of differential and integral equations as well as difference equations. In these established inequalities, Gronwall-Bellman-type inequalities are of particular importance as these inequalities provide explicit bounds for unknown functions, and much effort has been done for developing such inequalities (e.g., see [113] and the references therein). On the other hand, Hilger [14] initiated the theory of time scales as a theory capable containing both difference and differential calculus in a consistent way. Since then many authors have expounded on various aspects of the theory of dynamic equations on time scales (e.g., see [1517] and the references therein). In these investigations, integral inequalities on time scales have been paid much attention by many authors, and a lot of integral inequalities on time scales have been established (e.g., see [1826]), which have been designed to unify continuous and discrete analysis and play an important role in the research of qualitative and quantitative properties of solutions of certain dynamic equations on time scales. But to our knowledge, Gronwall-Bellman-type delay integral inequalities on time scales have been paid little attention in the literature so far. Recent results in this direction include the works of Li [27] and Ma and Pečarić [28] to our best knowledge. Furthermore, nobody has studied Gronwall-Bellman-type delay integral inequalities in two independent variables on time scales.

Our aim in this paper is to establish some new Gronwall-Bellman-type delay integral inequalities in two independent variables on time scales, which unify some known continuous and discrete analysis. New explicit bounds for unknown functions are obtained due to the presented inequalities. We will also present some applications for our results.

First we will give some preliminaries on time scales and some universal symbols for further use.

Throughout the paper, denotes the set of real numbers and + = [0, ), while denotes the set of integers. For two given sets G, H, we denote the set of maps from G to H by (G, H).

A time scale is an arbitrary nonempty closed subset of the real numbers. In this paper, 𝕋 denotes an arbitrary time scale. On 𝕋 we define the forward and backward jump operators σ ∈ (𝕋, 𝕋) and ρ ∈ (𝕋, 𝕋) by σ(t) = inf {s𝕋, s > t}  and  ρ(t) = sup {s𝕋, s < t}.

Definition 1.1. The graininess μ ∈ (𝕋, +) is defined by μ(t) = σ(t) − t.

Remark 1.2. Obviously, μ(t) = 0 if 𝕋 = while μ(t) = 1 if 𝕋 = .

Definition 1.3. A point t𝕋 is said to be left-dense if ρ(t) = t and t ≠ inf 𝕋, right-dense if σ(t) = t and t ≠ sup 𝕋, left-scattered if ρ(t) < t, and right-scattered if σ(t) > t.

Definition 1.4. The set 𝕋κ is defined to be 𝕋 if 𝕋 does not have a left-scattered maximum, otherwise it is 𝕋 without the left-scattered maximum.

Definition 1.5. A function f ∈ (𝕋, ) is called rd-continuous if it is continuous at right-dense points and if the left-sided limits exist at left-dense points, while f is called regressive if 1 + μ(t)f(t) ≠ 0. Crd denotes the set of rd-continuous functions, while denotes the set of all regressive and rd-continuous functions, and + = {ff, 1 + μ(t)f(t) > 0, ∀t𝕋}.

Definition 1.6. For some t𝕋κ and a function f ∈ (𝕋, ), the delta derivative of f is denoted by fΔ(t) and satisfies

(1.1)
where s𝔘, and 𝔘 is a neighborhood of t which can depend on ɛ.

Similarly, for some y𝕋κ and a function f ∈ (𝕋 × 𝕋, ), the partial delta derivative of f with respect to y is denoted by or and satisfies

(1.2)
where s𝔘, and 𝔘 is a neighborhood of y which can depend on ɛ.

Remark 1.7. If 𝕋 = , then fΔ(t) becomes the usual derivative f(t), while fΔ(t) = f(t + 1) − f(t) if 𝕋 = , which represents the forward difference.

Definition 1.8. For a, b𝕋 and a function f ∈ (𝕋, ), the Cauchy integral of f is defined by

(1.3)
where FΔ(t) = f(t),   t𝕋κ.

Similarly, for a, b𝕋 and a function f ∈ (𝕋 × 𝕋, ), the Cauchy partial integral of f with respect to y is defined by

(1.4)
where .

Definition 1.9. The cylinder transformation ξh is defined by

(1.5)
where Log is the principal logarithm function.

Definition 1.10. For p(x, y) ∈ with respect to y, the exponential function is defined by

(1.6)

Remark 1.11. If 𝕋 = , then for y the following formula holds:

(1.7)
If 𝕋 = , then, for y, and s < y.

The following two theorems include some known properties on the exponential function.

Theorem 1.12. If p(x, y) ∈ with respect to y, then the following conclusions hold:

  • (i)

    ep(y, y) ≡ 1 and e0(s, y) ≡ 1,

  • (ii)

    ep(s, σ(y)) = (1 + μ(y)p(x, y))ep(s, y),

  • (iii)

    if p+ with respect to y, then ep(s, y) > 0 for all s,   y𝕋,

  • (iv)

    if p+ with respect to y, then ⊖p+,

  • (v)

    ep(s, y) = 1/ep(y, s) = ep(y, s), where (⊖p)(x, y) = −(p(x, y)/1 + μ(y)p(x, y)).

Theorem 1.13. If p(x, y) ∈ with respect to y,   y0𝕋 is a fixed number, then the exponential function ep(y, y0) is the unique solution of the following initial value problem:

(1.8)

Theorems 1.12-1.13 are similar to [24, Theorems 5.1-5.2]. For more details about the calculus of time scales, we advise to refer to [29].

In the rest of this paper, for the convenience of notation, we always assume that , where x0,   y0𝕋κ, and furthermore assume that .

2. Main Results

We will give some lemmas for further use.

Lemma 2.1. Suppose that X𝕋0 is a fixed number and u(X, y),   b(X, y) ∈ Crd,   m(X, y) ∈ + with respect to y, m(X, y) ≥ 0; then

(2.1)
implies
(2.2)
where , and is the unique solution of the following IVP
(2.3)

The proof of Lemma 2.1 is similar to that of [24, Theorem 5.6], and we omit it here.

Lemma 2.2. Under the conditions of Lemma 2.1 and furthermore assuming that a(x, y) is nondecreasing in y for every fixed x,   b(x, y) ≡ 1, then one has

(2.4)

Proof. Since a(x, y) is nondecreasing in y for every fixed x, then from Lemma 2.1 we have

(2.5)
On the other hand, from [29, Theorems 2.39 and 2.36 (i)] we have .

Then collecting the above information we can obtain the desired inequality.

Lemma 2.3 (see [30].)Assume that a ≥ 0,   pq ≥ 0, and p ≠ 0, then for any K > 0

(2.6)

Theorem 2.4. Suppose that and a, b are nondecreasing. p, q, r, m are constants, and pq ≥ 0,   pr ≥ 0,   pm ≥ 0,     p ≠ 0.  τ1 ∈ (𝕋0, 𝕋),   τ1(x) ≤ x,    < α = inf {τ1(x), x𝕋0} ≤ x0. . ϕCrd(([α, x0]×[β, y0])⋂𝕋2, +). If for , u(x, y) satisfies the following inequality:

(2.7)
with the initial condition
(2.8)
then
(2.9)
where
(2.10)
(2.11)
(2.12)

Proof. Let the right side of (2.7) be v(x, y). Then

(2.13)
If τ1(x) ≥ x0 and τ2(y) ≥ y0, then , and since a, b are nondecreasing we have
(2.14)
If τ1(x) ≤ x0 or τ2(y) ≤ y0, then from (2.8) we have
(2.15)
From (2.14) and (2.15) we have
(2.16)
Fix X𝕋0, and let ; then
(2.17)
From Lemma 2.3, we have
(2.18)
So combining (2.17) and (2.18), it follows that
(2.19)
where B1(x, y), B2(x, y) are defined in (2.10) and (2.11), respectively. Considering , by application of Lemma 2.1, we have
(2.20)
Since X𝕋0 is arbitrary, then in fact (2.20) holds for all x𝕋0, that is,
(2.21)
Combining (2.13) and (2.21), we obtain
(2.22)
which is the desired inequality.

If we apply Lemma 2.2 instead of Lemma 2.1 at the end of the proof of Theorem 2.4, we obtain the following theorem.

Theorem 2.5. Suppose that u, f, g, h, a, p, q,   r, m, τ1, τ2, α, β, ϕ are defined as in Theorem 2.4. If that for satisfies the following inequality:

(2.23)
with the initial condition (2.8), then
(2.24)
where
(2.25)

From Theorems 2.4 and 2.5 we can obtain two direct corollaries.

Corollary 2.6. Under the conditions of Theorem 2.4, if, for , u(x, y) satisfies the following inequality:

(2.26)
with the initial condition (2.8) (p=1), then
(2.27)
where
(2.28)

Corollary 2.7. Under the conditions of Theorem 2.5, if, for , u(x, y) satisfies the following inequality:

(2.29)
with the initial condition (2.8) (p = 1), then
(2.30)
where
(2.31)

Theorem 2.8. Suppose that , f, g, h, τ1, τ2 are defined as in Theorem 2.4, and τ1(x) ≥ x0, τ2(y) ≥ y0. If, for satisfies the following inequality:

(2.32)
then u(x, y) ≡ 0.

The proof of Theorem 2.8 is similar to Theorem 2.4, and we omit it here.

Based on Theorem 2.4, we will establish a class of Volterra-Fredholm-type integral inequality on time scales.

Theorem 2.9. Suppose that are the same as in Theorem 2.4, and are two fixed numbers. If, for (x, y)∈([x0, M]⋂𝕋)×([y0, N]⋂𝕋),   u(x, y) satisfies the following inequality:

(2.33)
with the initial condition (2.8), then one has
(2.34)
provided that , where
(2.35)
(2.36)
(2.37)
(2.38)
(2.39)
(2.40)
(2.41)

Proof. Let the right side of (2.33) be v(x, y) and

(2.42)
Then
(2.43)
Similar to the process of (2.14)–(2.16) one has
(2.44)
Fix X ∈ [x0, M]⋂𝕋, and let x ∈ [x0, X]⋂𝕋,   y ∈ [y0, N]⋂𝕋. Then
(2.45)
Considering the structure of (2.45) is similar to (2.17), then following in a same manner as the process of (2.17)–(2.20) we can deduce
(2.46)
where are defined in (2.36) and (2.37), respectively.

Since X is selected from [x0, M]⋂𝕋 arbitrarily, then in fact (2.46) holds for all x𝕋0, that is,

(2.47)
where are defined in (2.38) and (2.39), respectively.

On the other hand, from (2.18), (2.42), and (2.44) we obtain

(2.48)
where λ is defined in (2.35). Then using (2.47) in (2.48) yields
(2.49)
which implies
(2.50)
Combining (2.43), (2.47), and (2.50) we can obtain the desired inequality (2.34).

In the proof of Theorem 2.9, if we let the right side of (2.33) be a(x, y) + v(x, y) in the first statement, then following in a same process as in Theorem 2.9 we obtain another bound on the function u(x, y), which is shown in the following theorem.

Theorem 2.10. Under the conditions of Theorem 2.9, if, for (x, y)∈([x0, M]⋂𝕋)×([y0, N]⋂𝕋), u(x, y) satisfies (2.33) with the initial condition (2.8), then the following inequality holds:

(2.51)
provided that , where
(2.52)

Finally, we will establish a more general inequality than that in Theorems 2.9-2.10. Consider the following inequality:
(2.53)
with the initial condition (2.8), where u, a, p, q, ϕ, α, β, τi, hi,   i = 1,2 are the same as in Theorem 2.4, are two fixed numbers. , and 0 ≤ L(s, t, x) − L(s, t, y) ≤ A(s, t, y)(xy) for xy ≥ 0, where .

Theorem 2.11. If, for (x, y)∈([x0, M]⋂𝕋)×([y0, N]⋂𝕋),   u(x, y) satisfies (2.53), then the following inequality holds:

(2.54)
provided that , where
(2.55)
(2.56)
(2.57)
(2.58)
(2.59)
(2.60)
(2.61)

Proof. Let the right side of (2.53) be v(x, y) and

(2.62)
Then
(2.63)
Similar to the process of (2.14)–(2.16) we have
(2.64)
Fix X ∈ [x0, M]⋂𝕋, and let x ∈ [x0, X]⋂𝕋,   y ∈ [y0, N]⋂𝕋. Then
(2.65)
From Lemma 2.3, we have
(2.66)
Combining (2.65) and (2.66), it follows that
(2.67)
where are defined in (2.56) and (2.57), respectively.

We notice the structure of (2.67) is similar to (2.19), so following in a same manner as in (2.19)–(2.21) we obtain

(2.68)
where are defined in (2.58) and (2.59), respectively.

On the other hand, from (2.62), (2.64), and (2.66) we have

(2.69)
where is defined in (2.55). Then using (2.68) in (2.69) yields
(2.70)
which implies
(2.71)
Combining (2.63), (2.68), and (2.71), we obtain the desired inequality (2.54).

Remark 2.12. The established above inequalities generalize many known results including both integral inequalities for continuous functions and discrete inequalities. For example, if we take 𝕋 = ,   p = q = 1,   g(x, y) = h(x, y) ≡ 0, then Theorem 2.4 reduces to [1, Theorem 2.2], which is one case of integral inequality for continuous function. If we take 𝕋 = ,   h(x, y) ≡ 0,   a(x, y) ≡ C, then Corollary 2.7 reduces to [2, Theorem 3 (c1)], which is another case of inequality for continuous function. If we take 𝕋 = ,   p = q = 1, g1(x, y) = g2(x, y) = f2(x, y) = h1(x, y) = h2(x, y) ≡ 0, then Theorem 2.10 reduces to [1, Theorem 2.2] with slight difference. If we take 𝕋 = ,   g1(x, y) = h1(x, y) = f2(x, y) = h2(x, y) ≡ 0,   τ1(x) = x,   τ2(y) = y, then Theorem 2.10 reduces to [3, Theorem 2.1], which is a discrete inequality.

Remark 2.13. Since 𝕋 is an arbitrary time scale, then if we take 𝕋 for some peculiar cases, such as 𝕋 = or 𝕋 = , we can deduce a series of corollaries according to Theorem 2.42.11. Due to the limited space, we omit them here.

3. Some Applications

In this section, we will present some applications for the results we have established previously. New explicit bounds for solutions of certain dynamic equations are derived in the first two examples, while the quantitative property of solutions is focused on in the final example.

Example 3.1. Consider the following delay dynamic differential equation:

(3.1)
with the initial condition
(3.2)
where , aCrd(𝕋0, ), , b is delta differential, and , p > 0 is a constant, . α, β, τ1, τ2 are the same as in Theorem 2.4.

Theorem 3.2. Suppose that u(x, y) is a solution of (3.1)-(3.2), |a(x) + b(y)| ≤ k(x, y), and |F(s, t, x, y)| ≤ f(s, t) | x|q+|y|, |W(ξ, η, x)| ≤ h(ξ, η) | x|m, where f, h, q, m are defined as in Theorem 2.4; then

(3.3)
where
(3.4)
and B2(x, y) is defined as in Theorem 2.4 (with g(x, y) ≡ 0).

Proof. The equivalent integral equation of (3.1) can be denoted by

(3.5)
Then
(3.6)
and a suitable application of Theorem 2.4 to (3.6) yields the desired inequality (3.3).

Theorem 3.3. Under the conditions of Theorem 3.2, one has

(3.7)
where B1, B2 are defined as in Theorem 3.2.

Proof. The desired inequality can be obtained by an application of Theorem 2.5 to (3.6).

Example 3.4. Consider the following delay dynamic integral equation:

(3.8)
with the initial condition
(3.9)
where , p > 0 is a constant, C = up(x0, y0), are two fixed numbers. . α, β, τ1, τ2 are the same as in Theorem 2.4.

Theorem 3.5. Suppose u(x, y) is a solution of (3.8)-(3.9) and |Fi(s, t, x, y)| ≤ L(s, t, |x|)+|y | ,    | Wi(ξ, η, x)| ≤ hi(ξ, η) | x|q,   i = 1,2, where L, hi,   i = 1,2,   q are defined the same as in Theorem 2.11; then the following inequality holds:

(3.10)
provided that , where are defined the same as in Theorem 2.11, and
(3.11)

Proof. From (3.8) we have

(3.12)
So by use of Theorem 2.11 we obtain the desired inequality (3.10).

Example 3.6. Consider the following delay dynamic integral equation:

(3.13)
where , . τ1, τ2 are the same as in Theorem 2.4.

Theorem 3.7. Assume that |F(s, t, u1, v1) − F(s, t, u2, v2)| ≤ f(s, t)|u1u2| + |v1v2|,    | W(s, t, u1) − W(s, t, u2)| ≤ h(s, t) | u1u2|, where f,   h are defined as in Theorem 2.4, and; furthermore, assume that τ1(x) ≥ x0,   τ2(y) ≥ y0, then (3.13) has at most one solution.

Proof. Suppose that u1(x, y),   u2(x, y) are two solutions of (3.13); then we have

(3.14)
Then a suitable application of Theorem 2.8 yields |u1(x, y) − u2(x, y)| ≤ 0, that is, u1(x, y) ≡ u2(x, y), and the proof is complete.

4. Conclusions

In this paper, we established some new Gronwall-Bellman type integral inequalities on time scales. As one can see, the presented results provide a handy tool in the quantitative as well as qualitative analysis of solutions of certain delay dynamic equations on time scales. The established inequalities unify some known continuous and discrete inequalities.

Acknowledgments

This work is supported by Natural Science Foundation of Shandong Province (ZR2009AM011) China and Specialized Research Fund for the Doctoral Program of Higher Education (20103705110003) China. The authors thank the referees very much for their careful comments and valuable suggestions on this paper.

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