- Research Article
- Open Access

# On Connection between Second-Order Delay Differential Equations and Integrodifferential Equations with Delay

- Leonid Berezansky
^{1}Email author, - Josef Diblík
^{2, 3}and - Zdenĕk Šmarda
^{3}

**2010**:143298

https://doi.org/10.1155/2010/143298

© Leonid Berezansky et al. 2010

**Received: **5 October 2009

**Accepted: **11 November 2009

**Published: **17 November 2009

## Abstract

## Keywords

- Integral Operator
- Qualitative Property
- Ballast Water
- Delay Differential Equation
- Integrodifferential Equation

## 1. Introduction and Preliminaries

The second order delay differential equation

attracts the attention of many mathematicians because of their significance in applications.

In particular, Minorsky [1] in 1962 considered the problem of stabilizing the rolling of a ship by an "activated tanks method" in which ballast water is pumped from one position to another. To solve this problem, he constructed several delay differential equations with damping described by (1.1).

Despite the obvious importance in applications, there are only few papers on delay differential equations with damping.

One of the methods used to study (1.1) is transforming the second-order delay differential equation to a first-order differential or integrodifferential equations with delay. A transformation of the type

where is a nonnegative function is used in [2]. The following result is a restriction of [2, Theorem ] to (1.1).

Proposition 1.1.

has a nonoscillatory solution, then (1.1) has a nonoscillatory solution, too.

Proposition 1.1 means that second order delay equation (1.1) is reduced to nonlinear inequality (1.3) and first order delay differential equation (1.4).

Now we will briefly describe the scheme of another transformation, different from the one used in [2] (in this explanation we omit exact assumptions related to the functions used, which are formulated later).

Consider an auxiliary equation

with the initial condition

It is known, see [3, 4], that the unique solution of (1.5), (1.6) has a form

where is the fundamental matrix of (1.5) and if .

If we denote , then (1.1) can be rewritten in the form

Applying (1.7) and equality to (1.8), we have the following equation

Then (1.1) is transformed into the integrodifferential equation with delay

Since (1.11) is a result of transforming (1.1), qualitative properties of (1.11) such as the existence and uniqueness of solutions, oscillation and nonoscillation, stability and asymptotic behavior can imply similar qualitative properties of (1.1).

The advantage of the suggested method in comparison with the method used in [2] is that a second order delay equation is reduced to one first-order integrodifferential delay equation while in [2] a second-order equation is reduced to a system of a nonlinear inequality and a linear delay equation.

Similar in a sense problems for delay difference equations were studied in [5, 6] as well.

This paper aims to investigate the problems of the existence, uniqueness and solution representation of (1.11). Problems related to oscillation/nonoscillation, stability and applications to second-order equations will be studied in our forthcoming papers. Throughout this paper, will denote the matrix or vector norm used.

## 2. Main Results

Together with (1.11) we consider an initial condition

We will assume that the following conditions hold:

(a1)For all , the elements , of the matrix function are measurable in the square , the elements , of the vector function are measurable in the interval ,

(a2) is a measurable scalar function satisfying , .

(a3)The initial function is a Borel bounded function.

A function is called a solution of the problem (1.11), (2.1) if it is a locally absolutely continuous function on , satisfies equation (1.11) on almost everywhere, and initial conditions (2.1) for .

Theorem 2.1.

Let conditions (a1)–(a3) hold. Then there exists a unique solution of problem (1.11), (2.1).

Proof.

It is sufficient to prove that there exists a unique solution of (1.11), (2.1) on the interval for any .

Denote

in the space of all Lebesgue integrable functions with the norm .

We have

is a unique solution of (1.11), (2.1).

Let be the zero matrix and the identity matrix.

Definition 2.2.

is called the fundamental matrix of (1.11). (Here is the partial derivative of with respect to its first argument.)

Theorem 2.3.

for where is defined by (2.5).

Proof.

where is the fundamental matrix of (1.11) is the solution of problem (2.4). For convenience, we will write instead of assuming that , if .

Equality (2.17) implies

## Declarations

### Acknowledgments

Leonid Berezansky was partially supported by grant 25/5 "Systematic support of international academic staff at Faculty of Electrical Engineering and Communication, Brno University of Technology" (Ministry of Education, Youth and Sports of the Czech Republic) and by grant 201/07/0145 of the Czech Grant Agency (Prague). Josef Diblík was supported by grant 201/08/0469 of the Czech Grant Agency (Prague), and by the Council of Czech Government grant MSM 00216 30503 and MSM 00216 30519. Zdeněk Šmarda was supported by the Council of Czech Government grant MSM 00216 30503 and MSM 00216 30529.

## Authors’ Affiliations

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## Copyright

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