Volume 2013, Issue 1 345697
Research Article
Open Access

Properties of Some Partial Dynamic Equations on Time Scales

Deepak B. Pachpatte

Corresponding Author

Deepak B. Pachpatte

Department of Mathematics, Dr. B. A. M. University, Aurangabad, Maharashtra 431004, India bamu.net

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First published: 01 July 2013
Academic Editor: Anjan Biswas

Abstract

The main objective of the paper is to study the properties of the solution of a certain partial dynamic equation on time scales. The tools employed are based on the application of the Banach fixed-point theorem and a certain integral inequality with explicit estimates on time scales.

1. Introduction

Recently, there has been a lot of interest in shown studying various properties of dynamic equations on time scales by various authors [111]. In this paper, we study some partial dynamic equations on time scales. Let n denote the n dimensional Euclidean space with appropriate norm |·|. In this, let denote the set of real numbers, the set of integers, and 𝕋 the arbitrary time scales. Let 𝕋1 and 𝕋2 be two time scales, and let Ω = 𝕋1 × 𝕋2. Let Crd denote the set of rd-continuous function. We assume basic understanding of time scales and notations. More information about time scales calculus can be found in [1214]. The partial delta derivative of z(x, y) for (x, y) ∈ Ω with respect to x, y, and xy is denoted by , , and .

Many physical systems can be modeled using dynamical systems on time scales. As response to the needs of diverse applications, many authors have studied qualitative properties of various equations on time scales [49, 11]. Motivated by the results in this paper, I consider the partial dynamic equation of the form
()
with the initial boundary conditions
()
for (x, y) ∈ Ω, where
()
fCrd(Ω × n × n × n, n), gCrd(Ω × Ω × n × n, n), α, βCrd(𝕋, n), and .

2. Preliminaries and Basic Inequality

We now give some basic definitions and notations about time scales. Define the jump operators σ, ρ : 𝕋𝕋 by
()
If σ(t) = t and σ(t) < t, then the point t𝕋 is left dense and left scattered. If ρ(t) = t and ρ(t) < t, then the point t𝕋 is right-dense and right-scattered. If 𝕋 has a right scattered minimum m, define 𝕋k : = 𝕋m; otherwise, 𝕋k : = 𝕋. If 𝕋 has a left-scattered maximum M, define 𝕋k : = 𝕋M; otherwise, 𝕋k : = 𝕋. The graininess function μ : 𝕋R+ = [0, ) is defined by μ(t) = σ(t) − t. We say that p : 𝕋 is regressive provided 1 + μ(t)p(t) ≠ 0 for all t𝕋. For f : 𝕋R and t𝕋k, the delta derivative of f at t denoted by fΔ(t) is the number (provided it exists) with the property that given any ϵ > 0, there is a neighborhood U of t such that
()
for all sU. For 𝕋 = R, fΔ(t) = f(t) the usual derivative; for 𝕋 = Z, the delta derivative is the forward difference operator, fΔ(t) = f(t + 1) − f(t). A function f : 𝕋R is right-dense continuous or rd-continuous provided it is continuous at right-dense points in 𝕋 and its left-sided limits exist (finite) and at left-dense points in 𝕋 and its left-sided limit exists (finite) at left-dense points in 𝕋. If 𝕋 = R, then f is rd-continuous if and only if f is continuous. It is known [12, Theorem 1.74] that f is right-dense continuous, there is a function F such that fΔ(t) = f(t) and
()
where a, b𝕋. Note that when 𝕋 = R, σ(t) = t, μ(t) = 0, fΔ = f, and , while then 𝕋 = Z, σ(t) = t + 1, μ(t) = 1, fΔ = Δf, and . We denote by the set of all regressive and rd-continuous functions and + = {p : 1 + μ(t)p(t) > 0  for  all  t𝕋}. For p, we define (see [12, Theorem 2.35]) the exponential function ep(·, t0) on time scale 𝕋 as the unique solution to the scalar initial value problem
()
If p+, then ep(t, t0) > 0 for all t𝕋 (see [12, Theorem 2.41]). As usual, the set of rd-continuous functions is denoted by Crd.
Denote by . For (t, s) ∈ Ω; the notation a(t, s) = O(b(t, s)); then there exists a constant q > 0 such that |a(t, s)/b(t, s)| ≤ q right hand neighbourhood. Let G be the space with function which are rd-continuous for (x, y) ∈ Ω and satisfy the condition
()
for (x, y) ∈ Ω, where λ > 0 is a constant. In space G, define the norm
()
The norm defined in (9) is clearly a Banach space. Then, (8) implies that there is a constant N ≥ 0 such that
()
Using (10), we observe that
()
The solution of (1) and (2) means a function u(x, y) ∈ Crd(Ω, n) satisfying (1) and (2). It is easy to observe that solution u(x, y) of initial boundary value problem (1) and (2) satisfies following dynamic integral equations on time scales:
()
for (x, y) ∈ Ω.

I need the following lemma proved in [15].

Lemma 1. Let u, a, fCrd(Ω, +) with a and f nondecreasing in each of the variables and g(t, t1, s, s2) ∈ Crd(Ω × Ω, +), a1 < s1 < t1, a2 < s2 < t2. If

()
for (t1, t2) ∈ Ω, then
()
for (t1, t2) ∈ Ω.

Now I prove the following integral inequality which is used in our results.

Lemma 2. Let w(x, y), a(x, y) ∈ Crd(Ω, +), p(x, y, s, t), b(x, y, s, t), , , , and let c ≥ 0 be a constant. If

()
for (x, y) ∈ Ω, then
()
()
for (x, y) ∈ Ω, where
()

Proof. Define a function z(x, y) by the right hand side of (15), then z(x, x0) = z(y0, y) = c, w(x, y) ≤ z(x, y), and z(x, y) is nondecreasing in x and y:

()
where A(x, y) is given by (18). Now, by application of Lemma 1, we get
()
Using (20) in w(x, y) ≤ z(x, y), we get the required inequality (16).

3. Existence and Uniqueness

Now our main results are as follows.

Theorem 3. Suppose that

  • (i)

    the function f, g in (1) satisfies the conditions

    ()

where k  (x, y) ∈ Crd  (Ω, +), h(x, y, m, n) ∈ Crd(Ω × Ω, +).

  • (ii)

    for λ as in (10),

    • (a)

      there exists a nonnegative constant γ such that γ < 1,

      ()

    • where

      ()

    • (b)

      there exists a nonnegative constant η such that

      ()

then, the initial boundary value problem (1) and (2) has a unique solution on Ω.

Proof. Let u(x, y) ∈ G, and define the operator S by

()
By delta differentiating (25) with respect to x and y, we get
()
Now, we show that Su maps G into itself and Su is rd-continuous on Ω.

From (25) and (26) and hypothesis, we have

()
From (27), it follows that SuG, thus proving that S maps G into itself.

Now, we verify that S is a contraction map. Let u(x, y), v(x, y) ∈ G. From (25) and (26) and using the hypotheses, we have

()
From (28), we have
()

Since γ < 1, it follows from Banach fixed-point theorem that S has unique fixed point in G. The fixed point of G is the solution of (1) and (2). This completes the proof.

Theorem 4. Suppose that function f, g in (1) satisfies the condition

()
where d is a nonnegative constant such that d < 1 and p(x, y, m, n), , , , ∈Crd(Ω × Ω, n). Then, initial boundary value problem (1) and (2) has at most one solution on Ω.

Proof. Let u1(x, y) and u2(x, y) be any two solutions of (1) and (2) and ; then by hypotheses we have

()
From (31), we have
()

Now, a suitable application of Lemma 2 to (32) yields

()
which implies that u1(x, y) = u2(x, y) for (x, y) ∈ Ω. Therefore, there is at most one solution of (1) and (2) on Ω.

4. Properties of Solutions

The following theorem contains estimates of solutions of (1) and (2).

Theorem 5. Assume that

()
()
()
where γ, η are nonnegative constants such that η < 1 and q(x, y, m, n), , , , ∈Crd  (Ω × Ω, n). If u(x, y) for (x, y) ∈ Ω is any solution of (1) and (2); then
()
where
()
for (x, y) ∈ Ω,
()

Proof. Since u(x, y) is a solution of (1) and (2) and by hypothesis, we have

()
From (40), we have
()
Now, a suitable application of Lemma 2 to (41) yields (37).

Remark 6. If the estimate obtained in (37) is bounded, then solution u(x, y) of (1) and (2) and also is bounded on Ω.

The following result deals with the continuous dependence of solution of (1) and (2).

Theorem 7. Assume that the functions f, g in (1) and (2) satisfy the conditions (30). Let u1(x, y) and u2(x, y) be the solutions of (1) with the given initial boundary conditions

()
()
respectively where β1, β2, τ1, τ2Crd  (𝕋, n),
()
where μ ≥ 0 is a constant. Then
()
for (x, y) ∈ Ω, where
()
where B(s, t) is defined by the right hand side of (18) replacing b(x, y, m, n) and p(x, y, m, n) by (1/(1 − d))p(x, y, m, n).

Proof. Let for (x, y) ∈ Ω. We have

()
From (47), we have
()

Now, a suitable application of Lemma 2 to (48) yields the bound (45) which shows the dependency of solution of (1) on the initial boundary conditions.

Now, we consider initial boundary value problem (1) and (2) and the corresponding initial boundary value problem

()
with the initial boundary conditions
()
where
()
GCrd(Ω × n × n × n, n), JCrd  (Ω × Ω × n × n, n), and .

Now, we present the result which deals with continuous dependence of solution of initial boundary value problem (1) and (2) on the functions involved therein.

Theorem 8. Assume that the functions f, g in (1) satisfy the conditions (30) and

()
where f, g, β, τ and are as in initial boundary value problem (1) and (2) and initial boundary value problem (49), (50), ϵ ≥ 0 is a constant, and v(x, y) is a solution of initial boundary value problem (49) and (50). Then, solution (1) and (2) depends continuously on the functions involved therein.

Proof. Let for (x, y) ∈ Ω. We have

()
From (53), we have
()
Now, a suitable application of Lemma 2 yields
()
for (x, y) ∈ Ω, where is given by (43). From (35), it follows that solution of initial boundary value problem (1) and (2) depends continuously on the functions involved therein.

Remark 9. In this paper, we have studied the existence and uniqueness of solution of (1) using Banach fixed-point theorem. Here, we have offered simple and concise proofs of properties of solutions of (1). I believeed results given will serve as a model for further investigations.

Acknowledgment

The author is grateful to the anonymous referee whose comments and suggestions helped the author to improve the text.

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