Open Access

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

Advances in Difference Equations20092010:143298

DOI: 10.1155/2010/143298

Received: 5 October 2009

Accepted: 11 November 2009

Published: 17 November 2009


The existence and uniqueness of solutions and a representation of solution formulas are studied for the following initial value problem: ,   ,   , , . Such problems are obtained by transforming second-order delay differential equations to first-order differential equations.

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.

If are Lebesgue measurable and locally essentially bounded, are Lebesgue measurable functions, , if , , there exists a locally absolutely continuous function such that the inequality
is valid for all sufficiently large , and the equation

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).


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


Then , and (1.11), (2.1) takes the form
Denote the characteristic function of the interval . We will assume that if . Since
we have
Hence problem (2.4) can be transformed into
We have
Finally, problem (2.4) has the form
where . Consider the linear integral operator

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

We have

Hence the integral operator is a compact Volterra operator and its spectral radius is equal to zero [4, 7, 8]. Then the integral equation (2.11) has a unique solution . Consequently

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

Let be the zero matrix and the identity matrix.

Definition 2.2.

For each , the solution of the problem

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

Theorem 2.3.

Let conditions (a1)–(a3) hold. Then the unique solution of (1.11), (2.1) can be represented in the form

for where is defined by (2.5).


In the proof we will use notation defined in the proof of Theorem 2.1. The existence and uniqueness of a solution of (1.11), (2.1) is a consequence of Theorem 2.1. Thus, we will only prove the solution representation formula (2.16). Problem (1.11), (2.1) is equivalent to (2.4). We need to show that the function

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

We consider the left-hand side of (2.4) if assuming to have the form (2.17). With the help of the last relation, we have
we obtain



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

Department of Mathematics, Ben-Gurion University of the Negev
Department of Mathematics and Descriptive Geometry, Faculty of Civil Engineering, Brno University of Technology
Department of Mathematics, Faculty of Electrical Engineering and Communication, Brno University of Technology


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© Leonid Berezansky et al. 2010

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