Novel Bounds for Solutions of Nonlinear Differential Equations ()
1. Introduction
The problem of estimating the norms of solutions to nonlinear systems of ordinary differential equations remains urgent due to extensive application of the latter in the description of real processes in many mechanical, physical and other nature systems. Usually, to obtain the estimates of norms of solutions to linear and weakly nonlinear equations, the Gronwall-Bellman lemma is applied (see, for example, [1] -[3] and bibliography therein). The development of the theory of nonlinear inequalities has substantially widened the possibilities for obtaining the estimates of norms of solutions to nonlinear systems and has given an impetus to their application in the qualitative theory of equations (see, for example, [4] -[6] ).
Both linear and nonlinear integral inequalities are efficiently used for the development of the direct Lyapunov method, in particular, for the investigation of motion boundedness and stability of nonlinear weakly connected systems [7] .
The present paper is aimed at obtaining new estimates of norms of solutions for some classes of nonlinear equations of perturbed motion. The paper is arranged as follows.
In Section 2 the statement of the problem is given in view of some results of papers [1] [3] .
Section 3 presents main results on obtaining the estimates of norms of solutions for some classes of nonlinear systems of differential equations. In this regard, several results from [8] are taken into account.
In Section 4 two application problems are considered: a problem on stabilization of solutions to affine system (cf. [8] ) and a problem on estimation of divergence of solutions at synchronization (cf. [9] ).
In Section 5 the possibilities of application of this approach for solution of modern problems of nonlinear dynamics and systems theory are discussed.
2. Statement of the Problem
Consider a nonlinear system of ordinary differential equations of perturbed motion
(1)
where
;
,
is an
-matrix with the elements continuous on any finite interval. It is assumed that solution
of problem (1) exists and is unique for all
and 
Equations of type (1) are found in many problems of mechanics (see, for example, [1] [10] and bibliography therein). Moreover, these equations may be treated as the ones describing the perturbation of the system of linear equations
(2)
In order to establish boundedness and stability conditions for solutions of system (1) it is necessary to estimate the norms of solutions under various types of restrictions on system (2) and vector-function of nonlinearities in system (1).
The purpose of this paper is to obtain estimates of norms of solutions to some classes of nonlinear ordinary differential Equations (1) in terms of nonlinear and pseudo-linear integral inequalities.
3. Main Results
First,we shall determine the estimate of the norm of solutions
of system (1) under the following assumptions:
A1. For all
there exists a nonnegative integrable function
such that

A2. For all
and
there exists a continuous nonnegative integrable function
,
, such that (cf. [11] )
![]()
for all
.
Here and elsewhere an Euclidian norm of the vector x and a spectral norm of the matrix consistent with it are used.
Theorem 1. For system (1) let conditions of assumptions
and
be satisfied, then for any solution
with the initial values
,
the inequality
(3)
holds for all
.
If there exist:
(a) a continuous and nonnegative function
for all
and
(b) a continuous, nonnegative and nondecreasing function
for
such that
![]()
then for all
the inequality
(4)
holds true, where
is a function converse with respect to the function
:
![]()
and the value
is determined by the correlation
![]()
(c) If, additionally, there exists a constant
such that
![]()
then inequality (4) is satisfied for all
, i.e.
for the values
.
Proof. Let the right-hand part of inequality (3) be equal
. Using inequality (3) and condition (b) of Theorem 1 we get
![]()
Since the function
is nondecreasing and
![]()
we get the inequality
![]()
Hence, by the Bihari lemma (see [10] , p. 110) we have
![]()
for all
. This implies estimate (4).
To prove the second assertion of Theorem 1 we note that the continuability condition for function
is the inequality
![]()
or
![]()
This inequality is satisfied for any
for which condition (c) of Theorem 1 holds true. Since
, we have
![]()
Hence it follows that for
the value
. This proves Theorem 1.
Further we shall consider system (1) under the following assumption.
A3. There exist a nonnegative integrable function
for all
and a constant
such that
![]()
for all
.
Theorem 2. For the system of Equations (1) let conditions of Assumptions
and
be satisfied. Then for the norm of solutions
the estimate
(5)
holds true for all
whenever
(6)
Proof. Let
be the solution of system of Equations (1) with the initial conditions
,
. Under conditions
and
Equation (1) yields the estimate of the norm of solution
in the form
(7)
We transform inequality (7) to the pseudo-linear form
(8)
and applying the Gronwall-Bellman lemma [1] arrive at the estimate
(9)
for all
.
Further, for estimation of the expression
![]()
the following approach is applied (cf. [8] ).
Designate
for all
and from inequality (9) obtain
(10)
Multiplying both parts of inequality (10) by the expression
![]()
we get
![]()
This implies that
![]()
Integrating the obtained inequality between the limits
and
we arrive at
![]()
Under condition (6) this estimate implies
![]()
Moreover, inequality (10) becomes
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This inequality yields estimate (5) for all
for which condition (6) is satisfied.
This completes the proof of Theorem 2.
Inequality (7) is a partial case of inequality (3) and its representation in pseudo-linear form (8) allows us to simplify the procedure of obtaining the estimate of norm of solutions to system (1).
Theorem 2 has a series of corollaries as applied to some classes of systems of ordinary differential equations.
Corollary 1. Consider system (1) for
for all ![]()
(11)
This is an essentially nonlinear system, i.e. a system without linear approximation. Such systems are found in the consideration of systems with dry friction, electroacoustic waveguides and in other problems. Systems with sector nonlinearity (see [12] ) are close to this type of systems.
If condition A3 is fulfilled with the function
such that
![]()
for any
,
,
, then
![]()
Applying to this inequality the same procedure as in the proof of Theorem 2 it is easy to show that if
![]()
for all
, then
(12)
for all
.
Comment 1. Estimate (12) is obtained as well by an immediate application of the Bihari lemma (see [10] ) to the inequality
![]()
with the function
,
,
.
Corollary 2. In system (1) let
, where
is an
-matrix continuous with respect to
.
Consider a system of non-autonomous linear equations with pseudo-linear perturbation
(13)
Assume that condition
is satisfied and there exists a nonnegative integrable function
such that
(14)
for all
.
Equation (13) implies that
(15)
Applying to inequality (15) the same procedure as in the proof of Theorem 2 we get the estimate
(16)
which holds true for the values of
for which
(17)
Comment 2. If in inequality (15) functions
for all
, then Theorem 1 yields the estimate (see [4] )
![]()
for all
, where
is determined by the formula
.
Corollary 3. In system (1) let
, where
for all
. Further we shall consider the system of nonlinear equations
(18)
where
are
-matrices with the elements continuous on any finite interval and
.
Assume that there exist nonnegative integrable on
functions
,
, such that
(19)
In view of (19) we get from (18) the inequality
(20)
Inequality (20) is presented in pseudo-linear form
![]()
Hence
(21)
We shall find the estimate of the expression ![]()
Inequality (21) implies that the estimate
![]()
is true.
Multiplying both parts of this inequality by the negative expression
![]()
we get
![]()
Summing up both parts of this inequality from
to
we find
![]()
Integration of this inequality between 0 and t results in the following inequality
![]()
From this inequality we find that
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Hence follows the estimate
(22)
which is valid for all
such that
![]()
Estimate (5) allows boundedness and stability conditions for solution of system (1) to be established in the following form.
Theorem 3. If conditions
and
of Theorem 2 are satisfied for all
and there exists a constant
such that
for all
, where
may depend on each solution, then the solu- tion
of system (1) is bounded.
Theorem 4. If conditions A1 and A3 of Theorem 2 are satisfied for all
and
for
, and for any
and
t0? 0 there exists a
such that if
, then the estimate
is satisfied for all
, then the zero solution of system (1) is stable.
The proofs of Theorems 3 and 4 follow immediately from the estimate of norm of solutions
in the form
of (5). The notations
and
mean that the right hand part of inequality (5) must sa-
tisfy these inequalities under appropriate initial conditions.
Similar assertions are valid for the systems of Equations (11), (13) and (18) in terms of estimates (12), (16) and (22).
4. Applications
4.1. Stabilization of Motions of Affine System
Consider an affine system with many controlling bodies
(23)
(24)
(25)
where
,
is an
-matrix with continuous elements on any finite interval,
is an
- matrix, the control vectors
for all
, B is an
-matrix and the control
, C is a constant
-matrix,
is a vector of the initial states of system (23). With regard to system (23) the following assumptions are made:
A4. Functions
,
, for all
.
A5. There exists a constant
-matrix
such that for the system
![]()
the fundamental matrix
satisfies the estimate
![]()
for
, where
and
are some positive constants.
A6. There exist constants
and
such that
![]()
for all
.
The following assertion takes place.
Theorem 5. Let conditions of assumptions
-
be satisfied and, moreover,
![]()
where
.
Then the controls
![]()
stabilize the motion of system (23) to the exponentially stable one.
Proof. Let the controls
and
be used to stabilize the motions of system (23). Besides, we have
![]()
and
(26)
In view of conditions of Theorem 5 we get from (26) the estimate of norm of solution of system (23) in the form
(27)
We transform inequality (27) to the form
(28)
Applying Corollary 3 to inequality (28) we get
![]()
for all
.
If condition
![]()
of Theorem 5 is satisfied, then
![]()
and for the norm of solution
we have the estimate
![]()
for all
, where
![]()
This completes the proof of Theorem 5.
4.2. Syncronization of Motions
The theory of motion synchronizations studies the systems of differential equations of the form (see [9] and bibliography therein)
(29)
where
,
is a function continuous with respect to
,
,
and periodic with respect to
with the period
, and
is a small parameter. Alongside system (29) we shall consider an adjoint system of equations
(30)
where
![]()
Assume that in the neighborhood of point
for sufficiently small value of
for any
the vector-function
and its partial derivatives are continuous. Designate
![]()
It is clear that the solutions of Equations (29) and (30) remain in the neighborhood
for
.
With allowance for
![]()
and
![]()
we compile the correlation
(31)
As it is shown in monograph [9] for the first and third summands in correlation (31) the following estimates hold true
(32)
(33)
To estimate the second summand we assume that there exist an integrable function
such that for any
![]()
![]()
and
such that
(34)
in the domain of values
and
.
In view of estimates (32)-(34) we find from (31)
(35)
for all
.
Let there exist
such that
(36)
for all
. Then the norm of divergence of solutions
and
under the same initial conditions is estimated as follows
(37)
for all
and for
.
Estimate (37) is obtained from inequality (35) by the application of Corollary 1.
Comment 3. If in estimate (34)
and
, then the application of the Gronwall-Bellman lemma to inequality (35) yields the estimate of divergence between solutions in the form [9]
![]()
for all
.
5. Concluding Remarks
In this paper the estimates of norms of solutions to differential equations of form (1), (11) and (13) are obtained in terms of nonlinear and pseudo-linear integral inequalities. This approach facilitates establishing the estimates of norms of solutions for some classes of systems of equations of perturbed motion found in various applied problems (see [11] [13] ). Efficiency of the obtained results is illustrated by two problems of nonlinear dynamics.
It is of interest to develop the obtained results in the investigation of solutions to dynamic equations on time scale (see [14] [15] ). In monograph [16] the integral inequalities on time scale form a basis of one of the methods of analysis of solutions to dynamic equations.