Research Article Stability in Terms of Two Measures for Nonlinear Impulsive

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Hindawi Publishing Corporation
Journal of Applied Mathematics
Volume 2013, Article ID 313029, 12 pages
http://dx.doi.org/10.1155/2013/313029
Research Article
Stability in Terms of Two Measures for Nonlinear Impulsive
Systems on Time Scales
Kexue Zhang1 and Xinzhi Liu2
1
2
School of Control Science and Engineering, Shandong University, Jinan 250061, China
Department of Applied Mathematics, University of Waterloo, Waterloo, ON, Canada N2L 3G1
Correspondence should be addressed to Xinzhi Liu; xzliu@uwaterloo.ca
Received 18 November 2012; Accepted 7 January 2013
Academic Editor: Qiru Wang
Copyright © 2013 K. Zhang and X. Liu. This is an open access article distributed under the Creative Commons Attribution License,
which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
We investigate some stability problems in terms of two measures for nonlinear dynamic systems on time scales with fixed moments
of impulsive effects. Sufficient conditions for (uniform) stability, (uniform) asymptotic stability, and instability in terms of two
measures are derived by using the method of Lyapunov functions. Our results include the existing results as special cases when
the time scale reduces to the set of real numbers. Particularly, our results provide stability criteria for impulsive discrete systems in
terms of two measures, which have not been investigated extensively. Two examples are presented to illustrate the efficiency of the
proposed results.
1. Introduction
It is well known that the theory of impulsive differential
equations provides a general framework for mathematical
modeling of many real world phenomena [1, 2]. In particular,
it serves as an adequate mathematical tool for studying
evolution processes that are subjected to abrupt changes in
their states. At the present time, the qualitative theory of
such equations has been extensively studied. Many results on
the stability and boundedness of their solutions are obtained
[1–4]. Due to the needs of applications, the concepts of
Lyapunov stability have given rise to many new notions,
for example, partial stability, conditional stability, eventual
stability, practical stability, and so on. A notion which unifies
and includes the above concepts of stability is the notion of
stability in terms of two measures which was initialed by
Movchan [5]. Since the publication of Salvadori’s paper [6],
this unified theory in terms of two measures became popular.
For a systematic introduction to the theory of stability in
terms of two measures, refer to [7].
On the other hand, a theory of time scales or calculus
on measure chains was introduced by Hilger in his Ph.D.
thesis [8] in 1988, with the purpose of incorporating both the
existing theory of dynamic systems on continuous and
discrete time scales, namely, time scale as arbitrary closed
subset of real numbers, and extending the existing theory to dynamic systems on generalized hybrid (continuous/discrete) time scales. The theory of time scales recently
has gained much attention and is undergoing rapid development. Recently, various work has been done on the stability
problem of dynamic systems on time scales [9–14]. For more
details about the theory of time scales, refer to [15–17].
Motivated by the above discussion, in this paper, we will
consider the stability problems in terms of two measures
for impulsive systems on time scales. Several new stability
criteria and instability criteria are obtained by using the
method of Lyapunov functions. As far as we know, there are
very few studies on stability analysis of impulsive discrete
systems in terms of two measures. Moreover, our results
can be applied to impulsive systems on other time scales in
addition to the set of integers and the set of real numbers.
The rest of this paper is organized as follows. In
Section 2, we introduce some basic knowledge of dynamic
systems on time scales. In Section 3, we formulate the
problem and present several definitions of stability and
instability in terms of two measures. In Section 4, several
2
Journal of Applied Mathematics
(β„Ž0 , β„Ž)-stability and instability criteria are established by
employing the Lyapunov function approach. For illustration
of our results, two examples are shown in Section 5. Finally,
some conclusions are drawn in Section 6.
2. Preliminaries
In this section, we briefly introduce some basic definitions
and results concerning time scales for later use.
Let R be the set of real numbers, R+ be the set of
nonnegative real numbers, Z be the set of integers, Z+ be
the set of nonnegative integers, N = {1, 2, . . .}, and T be an
arbitrary nonempty closed subset of R. We assume that T is
a topological space with relative topology induced from R.
Then, T is called a time scale.
Definition 1. The mappings 𝜎, πœƒ : T → T defined as
𝜎 (𝑑) = inf {𝑠 ∈ T : 𝑠 > t} ,
πœƒ (𝑑) = sup {𝑠 ∈ T : 𝑠 < 𝑑}
(1)
are called forward and backward jump operators, respectively.
A nonmaximal element 𝑑 ∈ T is called right-scattered (rs)
if 𝜎(𝑑) > 𝑑 and right-dense (rd) if 𝜎(𝑑) = 𝑑. A nonminimal
element 𝑑 ∈ T is called left-scattered (ls) if πœƒ(𝑑) < 𝑑 and leftdense (ld) if πœƒ(𝑑) = 𝑑. If T has a ls maximum π‘š, then we define
T π‘˜ = T \ {π‘š}, otherwise, T π‘˜ = T.
Definition 2. The graininess function πœ‡ : T → R+ is defined
by
πœ‡ (𝑑) = 𝜎 (𝑑) − 𝑑.
(2)
Definition 3. For 𝑦 : T → R and 𝑑 ∈ T π‘˜ , one defines the delta
derivative π‘¦Δ (𝑑) of 𝑦(𝑑), to be the number (when it exists) with
the property that for any πœ€ > 0, there is a neighborhood π‘ˆ of
𝑑 (i.e., π‘ˆ = (𝑑 − 𝛿, 𝑑 + 𝛿) β‹‚ T for some 𝛿 > 0) such that
󡄨
󡄨󡄨
󡄨󡄨𝑦 (𝜎 (𝑑)) − 𝑦 (𝑠) − π‘¦Δ (𝑑) (𝜎 (𝑑) − 𝑠)󡄨󡄨󡄨
󡄨
󡄨
≤ πœ€ |𝜎 (𝑑) − 𝑠| ,
∀𝑠 ∈ π‘ˆ.
(3)
A function 𝑓 : T → R is rd-continuous if it is continuous
at rd points in T and its left-side limits exist at ld points in
T. The set of rd-continuous functions 𝑓 : T → R will be
denoted by 𝐢rd = 𝐢rd (T, R). If 𝑓 is continuous at each rd
point and each ld point, 𝑓 is said to be continuous function
on T. If π‘Ž, 𝑏 ∈ T, then one defines the interval [π‘Ž, 𝑏] on T by
[π‘Ž, 𝑏] := {t ∈ T : π‘Ž ≤ 𝑑 ≤ 𝑏}. Open intervals and half-open
intervals can be defined similarly.
Definition 4. Let 𝑓 ∈ 𝐢rd . A function 𝑔 : T → R is called the
antiderivative of 𝑓 on T if it is differentiable on T and satisfies
π‘”Δ (𝑑) = 𝑓(𝑑) for all 𝑑 ∈ T. In this case, one defines
𝑑
∫ 𝑓 (𝑠) Δ𝑠 = 𝑔 (𝑑) − 𝑔 (π‘Ž) ,
π‘Ž
π‘Ž, 𝑑 ∈ T.
(4)
One says that a function 𝑝 : T → R is regressive if
1 + πœ‡(𝑑)𝑝(𝑑) =ΜΈ 0 for all 𝑑 ∈ T. The set of all regressive and
rd-continuous functions 𝑓 : T → R is denoted by 𝐢rd R =
𝐢rd R(T, R), and the set of all positively regressive elements
of 𝐢rd R is denoted by 𝐢rd R+ = 𝐢rd R+ (T, R) = {𝑝 ∈ 𝐢rd R :
1 + πœ‡(𝑑)𝑝(𝑑) > 0 for all 𝑑 ∈ T}.
Definition 5. If 𝑝 ∈ 𝐢rd R, then one defines the exponential
function on time scale T by
𝑑
𝑒𝑝 (𝑑, 𝑠) = exp (∫ πœ‰πœ‡(𝜏) (𝑝 (𝜏)) Δ𝜏) ,
𝑠
for 𝑑, 𝑠 ∈ T,
(5)
where the cylinder transformation
{ Log (1 + β„Žπ‘§) , β„Ž =ΜΈ 0,
πœ‰β„Ž (𝑧) = {
β„Ž
β„Ž = 0,
{𝑧,
where Log is the principal logarithm function.
(6)
It is known that π‘₯(𝑑) = 𝑒𝑝 (𝑑, 𝑑0 ) is the unique solution of
the initial value problem π‘₯Δ (𝑑) = 𝑝(𝑑)π‘₯(𝑑), π‘₯(𝑑0 ) = 1.
Remark 6. Let 𝛼 ∈ 𝐢rd R be a constant. If T = Z, then
𝑒𝛼 (𝑑, 𝑑0 ) = (1 + 𝛼)𝑑−𝑑0 for all 𝑑 ∈ T. If T = R, then 𝑒𝛼 (𝑑, 𝑑0 ) =
𝑒𝛼(𝑑−𝑑0 ) for all 𝑑 ∈ T.
Definition 7. One says that a function π‘š : T → R is rightnondecreasing at a point 𝑑 ∈ T provided
(i) if 𝑑 is rs, then π‘š(𝜎(𝑑)) ≥ π‘š(𝑑);
(ii) if 𝑑 is rd, then there is a neighborhood π‘ˆ of 𝑑 such that
π‘š (𝑠) ≥ π‘š (𝑑) ,
∀𝑠 ∈ π‘ˆ with 𝑠 > 𝑑.
(7)
Similarly, one says that π‘š is right-nonincreasing if above
in (i) π‘š(𝜎(𝑑)) ≤ π‘š(𝑑) and in (ii) π‘š(𝑠) ≤ π‘š(𝑑). If π‘š is rightnondecreasing (right-nonincreasing) at every 𝑑 ∈ T, one says
that π‘š is right-nondecreasing (right-nonincreasing) on T.
Lemma 8. Let π‘š ∈ 𝐢(T, R). Then π‘š(𝑑) is right-nondecreasing
(right-nonincreasing) on T if and only if 𝐷+ π‘šΔ (𝑑) ≥
0(𝐷+ π‘šΔ (𝑑) ≤ 0) for every 𝑑 ∈ T, where
π‘š (𝜎 (𝑑)) − π‘š (𝑑)
{
,
𝜎 (𝑑) > 𝑑,
{
{
πœ‡ (𝑑)
𝐷 π‘š (𝑑) = {
(8)
π‘š (𝑠) − π‘š (𝑑)
{
{lim sup
, 𝜎 (𝑑) = 𝑑.
𝑠−𝑑
{ 𝑠 → 𝑑+
Proof. The condition is obviously necessary. Let us prove that
it is sufficient. We only assume 𝐷+ π‘šΔ (𝑑) ≥ 0 for 𝑑 ∈ T as the
second statement can be shown similarly.
If 𝑑 is rs, then
+
Δ
𝐷+ π‘šΔ (𝑑) =
π‘š (𝜎 (𝑑)) − π‘š (𝑑)
≥ 0,
πœ‡ (𝑑)
(9)
and hence π‘š(𝜎(𝑑)) ≥ π‘š(𝑑).
Let now 𝑑 to be rd, and 𝑁 be a neighborhood of 𝑑. We need
to show that π‘š(𝑠) ≥ π‘š(𝑑) for 𝑠 > 𝑑 with 𝑠 ∈ 𝑁. This follows
directly from Lemma 1.1.1 in [7].
Thus the proof of the lemma is complete.
Journal of Applied Mathematics
3
3. Problem Formulation
Consider the following nonlinear impulsive system on time
scale T:
π‘₯Δ (𝑑) = 𝑓 (𝑑, π‘₯) ,
𝑑 =ΜΈ π‘‘π‘˜ , 𝑑 ∈ T,
Δπ‘₯ (𝑑) = πΌπ‘˜ (π‘₯ (𝑑)) ,
𝑑 = π‘‘π‘˜ , π‘˜ ∈ N,
(10)
π‘₯ (𝑑0+ ) = π‘₯0
under the following assumptions.
K = {𝛿 ∈ 𝐢(R+ , R+ ), strictly increasing and 𝛿(0) =
0};
𝑃𝐢K = {𝛿 : T × R+ → R+ , 𝛿(⋅, 𝑒) ∈ 𝑃𝐢 for each
𝑒 ∈ R+ and 𝛿(𝑑, ⋅) ∈ K for each 𝑑 ∈ T};
Γ = {β„Ž : T × R𝑛 → R+ , β„Ž(⋅, π‘₯) ∈ 𝑃𝐢 for each π‘₯ ∈
R𝑛 , β„Ž(𝑑, ⋅) ∈ 𝐢(R𝑛 , R+ ) for each 𝑑 ∈ T and inf β„Ž(𝑑, π‘₯) =
0};
𝜈0 = {𝑉 : T × R𝑛 → R+ , continuous on (π‘‘π‘˜−1 , π‘‘π‘˜ ] ×
R𝑛 , π‘˜ ∈ N, and for all π‘₯ ∈ R𝑛 and π‘˜ ∈ N,
lim(𝑑,𝑦) → (π‘‘π‘˜+ ,π‘₯) 𝑉(𝑑, 𝑦) = 𝑣(π‘‘π‘˜+ , π‘₯) exists}.
(a) T is a time scale with 𝑑0 ≥ 0 as minimal element and
no maximal element.
(b) {π‘‘π‘˜ } ∈ T, 𝑑0 < 𝑑1 < 𝑑2 < ⋅ ⋅ ⋅ < π‘‘π‘˜ < ⋅ ⋅ ⋅ and
limπ‘˜ → ∞ π‘‘π‘˜ = ∞.
(c) π‘₯ ∈ R𝑛 and Δπ‘₯(π‘‘π‘˜ ) = π‘₯(π‘‘π‘˜+ ) − π‘₯(π‘‘π‘˜− ). If π‘‘π‘˜ is rd point,
π‘₯(π‘‘π‘˜+ ) denotes the right limit of π‘₯ at π‘‘π‘˜ ; if π‘‘π‘˜ is rs point,
π‘₯(π‘‘π‘˜+ ) denotes the state of π‘₯ at π‘‘π‘˜ with the impulse. If π‘‘π‘˜
is ld point, π‘₯(π‘‘π‘˜− ) denotes the left limit of π‘₯ at π‘‘π‘˜ with
π‘₯(π‘‘π‘˜− ) = π‘₯(π‘‘π‘˜ ) if π‘‘π‘˜ is ls point. Here, we assume that
π‘₯(π‘‘π‘˜− ) = π‘₯(π‘‘π‘˜ ).
(d) 𝑓 : T × R𝑛 → R𝑛 is continuous in (π‘‘π‘˜−1 , π‘‘π‘˜ ] × R𝑛
for π‘˜ ∈ N, 𝑓(𝑑, 0) = 0, and for each π‘₯ ∈ R𝑛 , π‘˜ ∈ N,
lim(𝑑,𝑦) → (π‘‘π‘˜+ ,π‘₯) 𝑓(𝑑, 𝑦) = 𝑓(π‘‘π‘˜+ , π‘₯);
For 𝑉 ∈ 𝜈0 , (𝑑, π‘₯) ∈ (π‘‘π‘˜−1 , π‘‘π‘˜ ] × R𝑛 , π‘˜ ∈ N, we define the
upper right-hand Dini delta derivative of 𝑉(𝑑, π‘₯) relative to
(10) as follows:
Throughout this paper, we denote by π‘₯(𝑑) = π‘₯(𝑑; 𝑑0 , π‘₯0 ) the
solution of system (10) satisfying initial condition π‘₯(𝑑0+ ) = π‘₯0 .
Obviously, system (10) admits the trivial solution. Moreover,
𝑓 is assumed to satisfy necessary assumptions so that the
following initial value problems:
(i) β„Ž0 is finer than β„Ž if there exists a constant 𝜌 > 0 and
a function πœ‘ ∈ K such that β„Ž0 (𝑑, π‘₯) < 𝜌 implies
β„Ž(𝑑, π‘₯) ≤ πœ‘(β„Ž0 (𝑑, π‘₯));
(e) πΌπ‘˜ : R𝑛 → R𝑛 and πΌπ‘˜ (0) = 0.
π‘₯Δ = 𝑓 (𝑑, π‘₯) ,
𝑑 ∈ [𝑑0 , 𝑑1 ] ,
π‘₯ (𝑑0 ) = π‘₯0 ,
π‘₯Δ = 𝑓 (𝑑, π‘₯) ,
𝑑 ∈ (π‘‘π‘˜ , π‘‘π‘˜+1 ] ,
(11)
π‘₯ (π‘‘π‘˜+ ) = π‘₯ (π‘‘π‘˜ ) + πΌπ‘˜ (π‘₯ (π‘‘π‘˜ )) ,
have unique solutions π‘₯0 (𝑑), 𝑑 ∈ [𝑑0 , 𝑑1 ], and π‘₯π‘˜ (𝑑), 𝑑 ∈
(π‘‘π‘˜ , π‘‘π‘˜+1 ], π‘˜ ∈ N, respectively (e.g., see [17] for existence and
uniqueness results for dynamical systems on time scales.).
Thus, if we define
π‘₯0 (𝑑) , 𝑑 ∈ [𝑑0 , 𝑑1 ]
{
{
{
{
π‘₯1 (𝑑) , 𝑑 ∈ (𝑑1 , 𝑑2 ]
{
{
{
{
..
..
π‘₯ (𝑑; 𝑑0 , π‘₯0 ) = {
.
.
{
{
{
π‘₯π‘˜ (𝑑) , 𝑑 ∈ (π‘‘π‘˜ , π‘‘π‘˜+1 ]
{
{
{
{
..
..
.
.
{
𝐷+ π‘‰Δ (𝑑, π‘₯)
𝑉 (𝜎 (𝑑) , π‘₯ (𝜎 (𝑑))) − 𝑉 (𝑑, π‘₯ (𝑑))
{
,
{
{
πœ‡ (𝑑)
{
{
{
{
{
𝜎 (𝑑) > 𝑑,
={
𝑉
(𝑠,
π‘₯
+
−
𝑑)
𝑓
π‘₯
−
𝑉
π‘₯ (𝑑))
(𝑑)
(𝑠
(𝑑,
(𝑑)))
(𝑑,
{
{
,
lim sup
{
{
{
+
𝑠−𝑑
{
{ 𝑠→𝑑
𝜎 (𝑑) = 𝑑.
{
(13)
Definition 9. Let β„Ž0 , β„Ž ∈ Γ. Then one says that
(ii) β„Ž0 is weakly finer than β„Ž if there exists a constant 𝜌 >
0 and a function πœ‘ ∈ 𝑃𝐢K such that β„Ž0 (𝑑, π‘₯) < 𝜌
implies β„Ž(𝑑, π‘₯) ≤ πœ‘(𝑑, β„Ž0 (𝑑, π‘₯)).
Definition 10. Let 𝑉 ∈ 𝜈0 and β„Ž0 , β„Ž ∈ Γ. Then 𝑉(𝑑, π‘₯) is said
to be
(i) β„Ž-positive definite if there exist a 𝜌 > 0 and a function
𝑏 ∈ K such that β„Ž(𝑑, π‘₯) < 𝜌 implies 𝑏(β„Ž(𝑑, π‘₯)) ≤
𝑉(𝑑, π‘₯);
(ii) β„Ž0 -decrescent if there exist a 𝜌 > 0 and a function π‘Ž ∈
K such that β„Ž0 (𝑑, π‘₯) < 𝜌 implies 𝑉(𝑑, π‘₯) ≤ π‘Ž(β„Ž0 (𝑑, π‘₯));
(iii) β„Ž0 -weakly decrescent if there exist a 𝜌 > 0 and a
function π‘Ž ∈ 𝑃𝐢K such that β„Ž0 (𝑑, π‘₯) < 𝜌 implies
𝑉(𝑑, π‘₯) ≤ π‘Ž(𝑑, β„Ž0 (𝑑, π‘₯)).
Definition 11. The impulsive system (10) is said to be
(12)
(S1 ) (β„Ž0 , β„Ž)-stable, if for each πœ€ > 0, 𝑑0 ∈ T, there exists
a 𝛿 = 𝛿(𝑑0 , πœ€) > 0 such that β„Ž0 (𝑑0 , π‘₯0 ) < 𝛿 implies
β„Ž(𝑑, π‘₯(𝑑)) < πœ€, 𝑑 ≥ 𝑑0 for any solution π‘₯(𝑑) = π‘₯(𝑑; 𝑑0 , π‘₯0 )
of (10);
then it is easy to see that π‘₯(𝑑; 𝑑0 , π‘₯0 ) is the unique solution of
system (10).
Let us list the classes of functions and definitions for
convenience.
(S2 ) (β„Ž0 , β„Ž)-uniformly stable, if the 𝛿 in (S1 ) is independent
of 𝑑0 ;
𝑃𝐢 = {𝛿 : T → R+ , continuous on (π‘‘π‘˜−1 , π‘‘π‘˜ ] and
lim𝑑 → π‘‘π‘˜+ 𝛿(𝑑) = 𝛿(π‘‘π‘˜+ ) exists for π‘˜ ∈ N};
(S3 ) (β„Ž0 , β„Ž)-attractive, if for each πœ€ > 0, 𝑑0 ∈ T, there exist
two positive constants 𝛿 = 𝛿(𝑑0 , πœ€) and 𝑇 = 𝑇(𝑑0 , πœ€)
such that β„Ž0 (𝑑0 , π‘₯0 ) < 𝛿 implies β„Ž(𝑑, π‘₯(𝑑)) < πœ€, 𝑑 ≥
𝑑0 + 𝑇;
4
Journal of Applied Mathematics
(S4 ) (β„Ž0 , β„Ž)-uniformly attractive, if (S3 ) holds with 𝛿 and 𝑇
being independent of 𝑑0 ;
(S5 ) (β„Ž0 , β„Ž)-asymptotically stable, if (S1 ) and (S3 ) hold
simultaneously;
(S6 ) (β„Ž0 , β„Ž)-uniformly asymptotically stable, if (S2 ) and
(S4 ) hold together;
(S7 ) (β„Ž0 , β„Ž)-unstable, if (S1 ) fails to hold.
Let us establish, in this section, sufficient conditions for
(β„Ž0 , β„Ž)-(uniform) stability, (β„Ž0 , β„Ž)-(uniform) asymptotic stability, and (β„Ž0 , β„Ž)-instability properties of impulsive systems
(10) in the following subsections, respectively. Let
(14)
4.1. (β„Ž0 ,β„Ž)-(Uniform) Stability
(i) β„Ž, β„Ž0 ∈ Γ, and β„Ž0 is weakly finer than β„Ž;
Δ
𝐷 𝑉 (𝑑, π‘₯) ≤ π‘π‘˜ 𝑉 (𝑑, π‘₯) ,
(𝑑, π‘₯) ∈ 𝑆 (β„Ž, 𝜌) ,
Choose 𝛿 = min{𝛿0 , 𝛿1 , 𝛿2 }. Let (𝑑0 , π‘₯0 ) ∈ T × R𝑛 such that
β„Ž0 (𝑑0 , π‘₯0 ) < 𝛿 and π‘₯(𝑑) = π‘₯(𝑑; 𝑑0 , π‘₯0 ) be any solution of (10).
Then, from (17) to (20), we get
which implies β„Ž(𝑑0 , π‘₯0 ) < πœ€.
We now claim that, for every solution π‘₯(𝑑) = π‘₯(𝑑; 𝑑0 , π‘₯0 )
of (10), β„Ž0 (𝑑0 , π‘₯0 ) < 𝛿 implies
β„Ž (𝑑, π‘₯ (𝑑)) < πœ€,
𝑑 ≥ 𝑑0 .
(15)
β„Ž (𝑑, π‘₯ (𝑑)) < πœ€
(16)
where π‘₯π‘˜+ = π‘₯(π‘‘π‘˜+ ) and β„Ž(π‘‘π‘˜ , π‘₯π‘˜ ) < πœ€. Next, we will show that
there exists a 𝑑0 , π‘‘π‘˜ < 𝑑0 ≤ 𝑑∗ , such that
β„Ž (𝑑, π‘₯ (𝑑)) < 𝜌
(v) there exists a constant 𝜌1 , 0 < 𝜌1 < 𝜌, such that
β„Ž(𝑑, π‘₯) < 𝜌1 implies β„Ž(𝜎(𝑑), π‘₯(𝜎(𝑑))) < 𝜌;
(vi) there exists a constant 𝜌0 , 0 < 𝜌0 < 𝜌1 , such that
β„Ž(π‘‘π‘˜ , π‘₯π‘˜ ) < 𝜌0 implies β„Ž(π‘‘π‘˜+ , π‘₯π‘˜ + πΌπ‘˜ (π‘₯π‘˜ )) < 𝜌1 .
Then system (10) is (β„Ž0 , β„Ž)-stable.
Proof. Since 𝑉(𝑑, π‘₯) is β„Ž0 -weakly decrescent, there exist a
constant 𝛿0 > 0 and a function π‘Ž ∈ 𝑃𝐢K such that
if β„Ž (𝑑, π‘₯) < 𝜌.
if β„Ž0 (𝑑, π‘₯) < 𝛿1 .
Case 1. Let 𝑑 = inf{𝑑 ∈ (π‘‘π‘˜ , 𝑑∗ ], β„Ž(𝑑, π‘₯(𝑑)) ≥ 𝜌}. As β„Ž(π‘‘π‘˜+ , π‘₯π‘˜+ ) <
𝜌1 < 𝜌, we know that π‘‘π‘˜ < 𝑑 ≤ 𝑑∗ . If 𝑑 is left-dense,
from the selection of 𝑑, we know that there exists a left-hand
neighborhood π‘ˆπœ– = (𝑑 − πœ–, 𝑑) ⊂ (π‘‘π‘˜ , 𝑑∗ ] for some πœ– > 0, such
that 𝜌1 < β„Ž(𝑑, π‘₯(𝑑)) < 𝜌 for all 𝑑 ∈ π‘ˆπœ– . Then, we can choose
𝑑0 ∈ π‘ˆπœ– .
If 𝑑 is left-scattered, from the selection of 𝑑 and β„Ž(π‘‘π‘˜+ , π‘₯π‘˜+ ) <
𝜌1 , we know that π‘‘π‘˜ < πœƒ(𝑑) < 𝑑∗ and β„Ž(πœƒ(𝑑), π‘₯(πœƒ(𝑑))) < 𝜌. Here,
we claim that β„Ž(πœƒ(𝑑), π‘₯(πœƒ(𝑑))) ≥ 𝜌1 . If this is not true, that is,
β„Ž(πœƒ(𝑑), π‘₯(πœƒ(𝑑))) < 𝜌1 , form condition (v), we know that
β„Ž (𝑑, π‘₯ (𝑑)) = β„Ž (𝜎 (πœƒ (𝑑)) , π‘₯ (𝜎 (πœƒ (𝑑)))) < 𝜌,
(18)
which is a contradiction. Thus, 𝜌1 ≤ β„Ž(πœƒ(𝑑), π‘₯(πœƒ(𝑑))) < 𝜌.
Then, we can choose 𝑑0 = πœƒ(𝑑).
(19)
Case 2. If β„Ž(𝑑, π‘₯(𝑑)) < 𝜌 for all 𝑑 ∈ (π‘‘π‘˜ , 𝑑∗ ], then we can choose
𝑑0 = 𝑑∗ .
Hence, we can find a 𝑑0 , π‘‘π‘˜ < 𝑑0 ≤ 𝑑∗ , such that (25) holds.
By (i), there exist 𝛿1 > 0 and πœ‘ ∈ 𝑃𝐢K such that
β„Ž (𝑑, π‘₯) ≤ πœ‘ (𝑑, β„Ž0 (𝑑, π‘₯)) ,
(1) there exists a 𝑑∗ , π‘‘π‘˜ < 𝑑∗ ≤ 𝑑∗ , such that β„Ž(𝑑∗ , π‘₯(𝑑∗ )) ≥
𝜌;
(17)
There exists, in view of (ii), a function 𝑏 ∈ K such that
𝑏 (β„Ž (𝑑, π‘₯)) ≤ 𝑉 (𝑑, π‘₯) ,
for 𝑑 ∈ [𝑑0 , 𝑑0 ] .
(25)
(2) β„Ž(𝑑, π‘₯(𝑑)) < 𝜌 for all 𝑑 ∈ (π‘‘π‘˜ , 𝑑∗ ].
(iv) supπ‘˜∈Z+ {∏π‘˜π‘–=0 πœπ‘– 𝑒𝑐𝑖 (𝑑𝑖+1 , 𝑑𝑖 )} = 𝑀 < ∞ where 𝜍0 = 1;
if β„Ž0 (𝑑, π‘₯) < 𝛿0 .
(24)
To do this, we consider the following two cases:
where π‘₯π‘˜ = π‘₯(π‘‘π‘˜ ), π‘˜ ∈ N;
𝑉 (𝑑, π‘₯) ≤ π‘Ž (𝑑, β„Ž0 (𝑑, π‘₯)) ,
for 𝑑 ∈ [𝑑0 , π‘‘π‘˜ ] . (23)
β„Ž (π‘‘π‘˜+ , π‘₯π‘˜+ ) := β„Ž (π‘‘π‘˜+ , π‘₯π‘˜ + πΌπ‘˜ (π‘₯π‘˜ )) < 𝜌1 ,
πœ€ ≤ β„Ž (𝑑0 , π‘₯ (𝑑0 )) < 𝜌,
(iii) there exists 𝜍 ≥ πœπ‘˜ > 0, such that
(π‘‘π‘˜ , π‘₯π‘˜ ) ∈ 𝑆 (β„Ž, 𝜌) ,
(22)
If this is not true, then there exist a solution π‘₯(𝑑) with
β„Ž0 (𝑑0 , π‘₯0 ) < 𝛿 and a 𝑑∗ > 𝑑0 such that π‘‘π‘˜ < 𝑑∗ ≤ π‘‘π‘˜+1 , for
some π‘˜, satisfying
where π‘π‘˜ ≥ 0, π‘˜ ∈ Z+ ;
𝑉 (π‘‘π‘˜+ , π‘₯π‘˜ + πΌπ‘˜ (π‘₯π‘˜ )) ≤ πœπ‘˜ 𝑉 (π‘‘π‘˜ , π‘₯π‘˜ ) ,
(20)
Since 0 < πœ€ < 𝜌0 , it follows form condition (vi) that
(ii) 𝑉 ∈ 𝜈0 , 𝑉(𝑑, π‘₯) is β„Ž-positive definite on 𝑆(β„Ž, 𝜌), β„Ž0 weakly decrescent, locally Lipschtiz in π‘₯ for 𝑑 ∈ T which
is rd, and
𝑑 ∈ (π‘‘π‘˜ , π‘‘π‘˜+1 ) ,
max {1, 𝑀} π‘Ž (𝑑0 , 𝛿2 ) < 𝑏 (πœ€) .
β„Ž (𝑑∗ , π‘₯ (𝑑∗ )) ≥ πœ€,
Theorem 12. Assume that
+
πœ‘ (𝑑0 , 𝛿2 ) < 𝜌0 ,
𝑏 (β„Ž (𝑑0 , π‘₯0 )) ≤ 𝑉 (𝑑0 , π‘₯0 ) ≤ π‘Ž (𝑑0 , β„Ž0 (𝑑0 , π‘₯0 )) < 𝑏 (πœ€) , (21)
4. Main Results
𝑆 (β„Ž, 𝜌) = {(𝑑, π‘₯) ∈ T × R𝑛 : β„Ž (𝑑, π‘₯) < 𝜌} .
Let πœ€ ∈ (0, 𝜌0 ) and 𝑑0 ∈ T be given. There exists 𝛿2 =
𝛿2 (𝑑0 , πœ€) such that
(26)
Journal of Applied Mathematics
5
For 𝑑0 ≤ 𝑑 ≤ 𝑑0 and by conditions (ii) and (iii), we obtain
𝐷+ π‘‰Δ (𝑑, π‘₯) ≤ 𝑐𝑖 𝑉 (𝑑, π‘₯) ,
𝑑 ∈ (𝑑𝑖 , 𝑑𝑖+1 ) , 𝑑 ≤ 𝑑0 ,
𝑉 (𝑑𝑖+ , π‘₯𝑖 + 𝐼𝑖 (π‘₯𝑖 )) ≤ πœπ‘– 𝑉 (𝑑𝑖 , π‘₯𝑖 ) ,
𝑑0 < 𝑑𝑖 < 𝑑0 .
(27)
(28)
𝑑 ∈ [𝑑0 , 𝑑1 ] .
(29)
To do this, we apply the induction principle ([17], Theorem
1.7) on [𝑑0 , 𝑑1 ] to the statement
𝐴 (𝑑) : 𝑉 (𝑑, π‘₯) ≤ 𝑒𝑐0 (𝑑, 𝑑0 ) 𝑉 (𝑑0 , π‘₯0 ) .
(30)
(1) The statement 𝐴(𝑑0 ) is true since 𝑒𝑐0 (𝑑0 , 𝑑0 )𝑉(𝑑0 , π‘₯0 ) =
𝑉(𝑑0 , π‘₯0 ).
(2) Let 𝑑 be rs and 𝐴(𝑑) be true. We have to prove that
𝐴(𝜎(𝑑)) is true.
By the definition of upper right-hand derivative, we see
that
𝐷+ π‘‰Δ (𝑑, π‘₯) =
𝑉 (𝑑, π‘₯) ≤ 𝑒𝑐𝑖 (𝑑, 𝑑𝑖 ) 𝑉 (𝑑𝑖+ , π‘₯ (𝑑𝑖+ )) ,
for 𝑑 ∈ (𝑑𝑖 , 𝑑𝑖+1 ] , 𝑑 ≤ 𝑑0 .
(35)
Then, by (28), (35), and (20), we obtain
By (27), we will show that
𝑉 (𝑑, π‘₯) ≤ 𝑒𝑐0 (𝑑, 𝑑0 ) 𝑉 (𝑑0 , π‘₯0 ) ,
Hence, we conclude that (29) is true.
Similarly, we can prove that
𝑉 (𝜎 (𝑑) , π‘₯ (𝜎 (𝑑))) − 𝑉 (𝑑, π‘₯ (𝑑))
πœ‡ (𝑑)
𝑉 (𝑑0 , π‘₯ (𝑑0 )) ≤ π‘’π‘π‘˜ (𝑑0 , π‘‘π‘˜ ) 𝑉 (π‘‘π‘˜+ , π‘₯ (π‘‘π‘˜+ ))
≤ π‘’π‘π‘˜ (𝑑0 , π‘‘π‘˜ ) πœπ‘˜ 𝑉 (π‘‘π‘˜ , π‘₯ (π‘‘π‘˜ ))
+
+
, π‘₯ (π‘‘π‘˜−1
))
≤ π‘’π‘π‘˜ (𝑑0 , π‘‘π‘˜ ) πœπ‘˜ π‘’π‘π‘˜−1 (π‘‘π‘˜ , π‘‘π‘˜−1 ) 𝑉 (π‘‘π‘˜−1
≤ ⋅⋅⋅
≤ π‘’π‘π‘˜ (𝑑0 , π‘‘π‘˜ ) πœπ‘˜ π‘’π‘π‘˜−1 (π‘‘π‘˜ , π‘‘π‘˜−1 ) πœπ‘˜−1 ⋅ ⋅ ⋅ 𝑒𝑐1 (𝑑2 , 𝑑1 )
× πœ1 𝑒𝑐0 (𝑑1 , 𝑑0 ) 𝑉 (𝑑0 , π‘₯0 )
π‘˜
(31)
≤ 𝑐0 𝑉 (𝑑, π‘₯) ,
≤ ∏πœπ‘– 𝑒𝑐𝑖 (𝑑𝑖+1 , 𝑑𝑖 ) 𝑉 (𝑑0 , π‘₯0 ) ≤ 𝑀𝑉 (𝑑0 , π‘₯0 )
𝑖=0
≤ π‘€π‘Ž (𝑑0 , β„Ž0 (𝑑0 , π‘₯0 )) ≤ π‘€π‘Ž (𝑑0 , 𝛿) < 𝑏 (πœ€)
then
(36)
𝑉 (𝜎 (𝑑) , π‘₯ (𝜎 (𝑑))) ≤ (1 + 𝑐0 πœ‡ (𝑑)) 𝑉 (𝑑, π‘₯)
= 𝑒𝑐0 (𝜎 (𝑑) , 𝑑) 𝑉 (𝑑, π‘₯)
≤ 𝑒𝑐0 (𝜎 (𝑑) , 𝑑) 𝑒𝑐0 (𝑑, 𝑑0 ) 𝑉 (𝑑0 , π‘₯0 )
that is, 𝑉(𝑑0 , π‘₯(𝑑0 )) < 𝑏(πœ€). Thus, by (18) and (25),
(32)
which implies that 𝐴(𝜎(𝑑)) is true.
(3) Let 𝑑 be rd, 𝐴(𝑑) be true and 𝑁 be a neighborhood of
𝑑. We need to show that 𝐴(𝑠) is true for s > 𝑑, 𝑠 ∈ 𝑁. By (27)
and Remark 6, we get
(33)
= 𝑒𝑐0 (𝑠, 𝑑0 ) 𝑉 (𝑑0 , π‘₯0 )
which implies that 𝐴(𝑠) is true.
(4) Let 𝑑 be ld and 𝐴(𝑠) be true for all 𝑠 < 𝑑. We need to
show that 𝐴(𝑑) is true. By the continuous property of function
𝑉 and the exponential function, it follows that
𝑠→𝑑
𝑠→𝑑
= 𝑒𝑐0 (𝑑, 𝑑0 ) 𝑉 (𝑑0 , π‘₯0 )
which implies that 𝐴(𝑑) is true.
(i)∗ h0 is finer than β„Ž;
(ii)∗ V(t, x) is β„Ž0 -decrescent.
Proof. From conditions (i)∗ and (ii)∗ , the number 𝛿 in the
proof of Theorem 12 can be chosen independent of 𝑑0 . Then
following the same reasoning of Theorem 12, we can get
the (β„Ž0 , β„Ž)-uniform stability of system (10). The details are
omitted.
If π‘π‘˜ ≡ 0 in condition (ii) of the previous theorems, then
the Lyapunov function 𝑉 is monotone along the solutions of
system (10) in each impulsive intervals. In this case, we have
the following conservative result.
Corollary 14. Assume that
𝑉 (𝑑, π‘₯) = lim− 𝑉 (𝑠, π‘₯ (𝑠))
≤ lim− 𝑒𝑐0 (𝑠, 𝑑0 ) 𝑉 (𝑑0 , π‘₯0 )
Theorem 13. Assume that all conditions of Theorem 12 hold
with the following changes:
Then, system (10) is (β„Ž0 , β„Ž)-uniformly stable.
𝑉 (𝑠, π‘₯ (𝑠)) ≤ 𝑒𝑐0 (𝑠−𝑑) 𝑉 (𝑑, π‘₯)
= 𝑒𝑐0 (𝑠, 𝑑) 𝑒𝑐0 (𝑑, 𝑑0 ) 𝑉 (𝑑0 , π‘₯0 )
(37)
which is a contradiction. Therefore (22) is true and system
(10) is (β„Ž0 , β„Ž)-stable.
= 𝑒𝑐0 (𝜎 (𝑑) , 𝑑0 ) 𝑉 (𝑑0 , π‘₯0 )
≤ 𝑒𝑐0 (𝑠−𝑑) 𝑒𝑐0 (𝑑, 𝑑0 ) 𝑉 (𝑑0 , π‘₯0 )
𝑏 (πœ€) ≤ 𝑏 (β„Ž (𝑑0 , π‘₯ (𝑑0 ))) ≤ 𝑉 (𝑑0 , π‘₯ (𝑑0 )) < 𝑏 (πœ€)
(34)
(i) β„Ž0 , β„Ž ∈ Γ, 𝑉 ∈ 𝜈0 , 𝑉(𝑑, π‘₯) is β„Ž-positive definite on
𝑆(β„Ž, 𝜌), locally Lipschtiz in π‘₯ for each 𝑑 ∈ T which is
rd, and 𝐷+ π‘‰Δ (𝑑, π‘₯) ≤ 0 for 𝑑 =ΜΈ π‘‘π‘˜ and (𝑑, π‘₯) ∈ 𝑆(β„Ž, 𝜌);
(ii) 𝑉(π‘‘π‘˜+ , π‘₯π‘˜ + πΌπ‘˜ (π‘₯π‘˜ )) − 𝑉(π‘‘π‘˜ , π‘₯π‘˜ ) ≤ π‘‘π‘˜ 𝑉(π‘‘π‘˜ , π‘₯π‘˜ ) for
(π‘‘π‘˜ , π‘₯π‘˜ ) ∈ 𝑆(β„Ž, 𝜌), where π‘‘π‘˜ ≥ 0 and ∑∞
𝑖=1 𝑑𝑖 < ∞,
6
Journal of Applied Mathematics
and conditions (v), (vi) of Theorem 12 hold. Then
(A) if, in addition, β„Ž0 is weakly finer than β„Ž, and 𝑉(𝑑, π‘₯) is
β„Ž0 -weakly decrescent, then system (10) is (β„Ž0 , β„Ž)-stable;
(B) if, in addition, β„Ž0 is finer than β„Ž, and 𝑉(𝑑, π‘₯) is β„Ž0 decrescent, then system (10) is (β„Ž0 , β„Ž)-uniformly stable.
Proof. Notice
π‘˜
sup {∏πœπ‘– 𝑒𝑐𝑖 (𝑑𝑖+1 , 𝑑𝑖 )}
π‘˜∈Z+
𝑖=0
π‘˜
∞
𝑖=0
𝑖=1
(38)
where 𝑑0 = 0. Then, by Theorems 12 and 13, the result holds.
Remark 15. The continuous version of Corollary 14 with π‘‘π‘˜ ≡
0, π‘˜ ∈ N, can be found in [7], while the discrete one for
impulsive discrete systems is brand new, and the discrete
version of Corollary 14 with 𝑉(π‘‘π‘˜+ , π‘₯π‘˜ + πΌπ‘˜ (π‘₯π‘˜ )) = 𝑉(π‘‘π‘˜ , π‘₯(π‘‘π‘˜ )),
π‘˜ ∈ N, reduces to Theorems 3.1 and 3.2 in [18] for discrete
systems with no impulses.
4.2. (β„Ž0 ,β„Ž)-(Uniform) Asymptotic Stability
Theorem 16. Assume that conditions (v), (vi) of Theorem 12
and condition (i) of Corollary 14 hold and the following
conditions are satisfied:
(i) β„Ž0 is weakly finer than β„Ž, and 𝑉(𝑑, π‘₯) is β„Ž0 -weakly
decrescent;
(ii) 𝑉(π‘‘π‘˜+ , π‘₯π‘˜ + πΌπ‘˜ (π‘₯π‘˜ )) − 𝑉(π‘‘π‘˜ , π‘₯π‘˜ ) ≤ −πœ† π‘˜ πœ“(𝑉(π‘‘π‘˜ , π‘₯π‘˜ )) for
(π‘‘π‘˜ , π‘₯π‘˜ ) ∈ 𝑆(β„Ž, 𝜌), where πœ† π‘˜ ≥ 0, ∑∞
π‘˜=1 πœ† π‘˜ = ∞, πœ“ :
R+ → R+ , πœ“(0) = 0 and πœ“(𝑠) > 0 if 𝑠 > 0.
Then system (10) is (β„Ž0 , β„Ž)-asymptotically stable.
Proof. By Theorem 12, system (10) is (β„Ž0 , β„Ž)-stable. Thus, for
𝜌 > 0, there exists 𝛿 = 𝛿(𝑑0 , 𝜌) > 0 such that β„Ž0 (𝑑0 , π‘₯0 ) < 𝛿
implies β„Ž(𝑑, π‘₯) < 𝜌, 𝑑 ≥ 𝑑0 . To prove the theorem, it remains
to show that lim𝑑 → ∞ β„Ž(𝑑, π‘₯(𝑑)) = 0.
Let π‘š(𝑑) = 𝑉(𝑑, π‘₯(𝑑)). Then it follows from assumptions
that π‘š(𝑑) is right-nonincreasing and bounded from below,
and consequently lim𝑑 → ∞ π‘š(𝑑) = πœ” ≥ 0 exists. If πœ” > 0
for some solution π‘₯(𝑑) = π‘₯(𝑑; 𝑑0 , π‘₯0 ) of (10), we let 𝛾 =
minπœ”≤𝑠≤π‘š(𝑑0 ) πœ“(𝑠). Then, by condition (ii), we have
π‘š (π‘‘π‘˜+ ) − π‘š (π‘‘π‘˜ ) ≤ −πœ† π‘˜ πœ“ (π‘š (π‘‘π‘˜ )) ≤ −πœ† π‘˜ 𝛾.
(39)
Thus we obtain from (39) that
Theorem 17. Let conditions (v), (vi) of Theorem 12 hold and
assume that
(ii) there exists a function 𝑉 ∈ 𝜈0 such that 𝑉(𝑑, π‘₯) is locally
Lipschtiz in π‘₯ for each 𝑑 ∈ T which is rd, β„Ž-positive
definite on 𝑆(β„Ž, 𝜌), β„Ž0 -weakly decrescent and
𝐷+ π‘‰Δ (𝑑, π‘₯) ≤ −𝑐 (π‘Š (𝑑, π‘₯)) ,
≤ π‘š (π‘‘π‘˜−1 ) − πœ† π‘˜−1 𝛾 − πœ† π‘˜ 𝛾
(40)
where 𝑐 ∈ K, π‘Š ∈ 𝜈0 ;
(iii) 𝑉(π‘‘π‘˜+ , π‘₯π‘˜ + πΌπ‘˜ (π‘₯π‘˜ )) − 𝑉(π‘‘π‘˜ , π‘₯π‘˜ ) ≤ π‘‘π‘˜ 𝑉(π‘‘π‘˜ , π‘₯π‘˜ ), (π‘‘π‘˜ , π‘₯π‘˜ ) ∈
𝑆(β„Ž, 𝜌), where π‘‘π‘˜ ≥ 0 and ∑∞
𝑖=1 𝑑𝑖 < ∞;
(iv) π‘Š(𝑑, π‘₯) is β„Ž-positive definite on 𝑆(β„Ž, 𝜌), locally Lipschtiz
in π‘₯ for every 𝑑 ∈ T which is rd and
𝐷+ π‘ŠΔ (𝑑, π‘₯) ≤ 0,
𝑑 =ΜΈ π‘‘π‘˜ , (𝑑, π‘₯) ∈ 𝑆 (β„Ž, 𝜌) ,
π‘Š (π‘‘π‘˜+ , π‘₯π‘˜ + πΌπ‘˜ (π‘₯π‘˜ )) − π‘Š (π‘‘π‘˜ , π‘₯π‘˜ )
≤ π‘‘π‘˜ π‘Š (π‘‘π‘˜ , π‘₯π‘˜ ) ,
𝑗=1
(42)
(π‘‘π‘˜ , π‘₯π‘˜ ) ∈ 𝑆 (β„Ž, 𝜌) ,
where π‘‘π‘˜ ≥ 0 and ∑∞
𝑖=1 𝑑𝑖 < ∞.
Then system (10) is (β„Ž0 , β„Ž)-asymptotically stable.
Proof. From Corollary 14, it follows that system (10) is (β„Ž0 , β„Ž)stable. Thus, for 𝜌 > 0, there exists 𝛿 = 𝛿(𝑑0 , 𝜌) > 0 such
that β„Ž0 (𝑑0 , π‘₯0 ) < 𝛿 implies β„Ž(𝑑, π‘₯) < 𝜌, 𝑑 ≥ 𝑑0 . To prove the
theorem, it remains to show that for every solution π‘₯(𝑑) of
(10) with β„Ž0 (𝑑0 , π‘₯0 ) < 𝛿, lim𝑑 → ∞ β„Ž(𝑑, π‘₯) = 0.
Suppose that this is not true. Then there exists a sequence
{πœ‰π‘– }∞
𝑖=1 diverging to ∞ as 𝑖 → ∞ and such that β„Ž(πœ‰π‘– , π‘₯(πœ‰π‘– )) ≥
π‘Ÿ (𝑖 ∈ N) for some positive number π‘Ÿ. From condition (iv), we
know that there exists a function 𝑏 ∈ K such that 𝑏(β„Ž(𝑑, π‘₯)) ≤
π‘Š(𝑑, π‘₯), if β„Ž(𝑑, π‘₯) < 𝜌. Then
𝑖 ∈ N.
(43)
For any given 𝑑 ∈ T, there exists a 𝑖 > 0 such that 𝑑 ∈
(πœ‰π‘– , πœ‰π‘–+1 ]. Then for πœ‰π‘–+1 , there exists a π‘˜ > 0 such that πœ‰π‘–+1 ∈
(π‘‘π‘˜ , π‘‘π‘˜+1 ]. If π‘‘π‘˜ < 𝑑 ≤ π‘‘π‘˜+1 , from (43) and condition (iv), we
have
π‘˜
≤ π‘š (𝑑1 ) − 𝛾 ∑πœ† 𝑗 ,
(41)
𝑑 =ΜΈ π‘‘π‘˜ , (𝑑, π‘₯) ∈ 𝑆 (β„Ž, 𝜌) ,
π‘Š (πœ‰π‘– , π‘₯ (πœ‰π‘– )) > 𝑏 (π‘Ÿ) ,
+
π‘š (π‘‘π‘˜+ ) ≤ π‘š (π‘‘π‘˜ ) − πœ† π‘˜ 𝛾 ≤ π‘š (π‘‘π‘˜−1
) − πœ†π‘˜π›Ύ
≤ ⋅⋅⋅
In the following theorems, two auxiliary functions of
class 𝜈0 are used to investigate the (β„Ž0 , β„Ž)-asymptotic stability
property of system (10).
(i) β„Ž0 , β„Ž ∈ Γ and β„Ž0 is weakly finer than β„Ž;
= sup {∏ (1 + 𝑑𝑖 )} ≤ ∏ (1 + 𝑑𝑖 ) < ∞,
π‘˜∈Z+
which implies, in view of the assumption ∑π‘˜π‘—=1 πœ† 𝑗 = ∞, that
limπ‘˜ → ∞ π‘š(π‘‘π‘˜+ ) = −∞. This is a contradiction. Thus we must
have πœ” = 0 and consequently lim𝑑 → ∞ β„Ž(𝑑, π‘₯(𝑑)) = 0. Hence
system (10) is (β„Ž0 , β„Ž)-attractive and the proof is complete.
π‘Š (𝑑, π‘₯) ≥ π‘Š (πœ‰π‘–+1 , π‘₯ (πœ‰π‘–+1 )) > 𝑏 (π‘Ÿ) ≥
𝑏 (π‘Ÿ)
,
𝑀0
(44)
Journal of Applied Mathematics
7
where 𝑀0 = ∏∞
𝑗=1 (1 + 𝑑𝑗 ) < ∞. If π‘‘π‘˜−1 < 𝑑 ≤ π‘‘π‘˜ , we have
where 𝑀 = ∏∞
𝑗=1 (1 + 𝑑𝑗 ) < ∞. This is a contradiction, hence
lim𝑑 → ∞ β„Ž(𝑑, π‘₯) = 0. Theorem 17 is proved.
π‘Š (𝑑, π‘₯) ≥ π‘Š (π‘‘π‘˜ , π‘₯π‘˜ )
1
≥
1 + π‘‘π‘˜
π‘Š (π‘‘π‘˜+ , π‘₯ (π‘‘π‘˜+ )) >
1
1 + π‘‘π‘˜
𝑏 (π‘Ÿ) ≥
𝑏 (π‘Ÿ) (45)
.
𝑀0
In Theorem 17, the function may have a special form. In
the case when π‘Š(𝑑, π‘₯) = 𝑉(𝑑, π‘₯) and π‘‘π‘˜ = π‘‘π‘˜ , π‘˜ ∈ N, we
deduce the following corollary.
(46)
Corollary 18. Let conditions (v), (vi) of Theorem 12 hold and
assume that
Following this procedure, we conclude that
𝑏 (π‘Ÿ)
,
π‘Š (𝑑, π‘₯) >
𝑀0
𝑑 ∈ T.
Let
𝑑
𝐿 (𝑑, π‘₯) = 𝑉 (𝑑, π‘₯) + ∫ 𝑐 (π‘Š (𝑠, π‘₯ (𝑠))) Δ𝑠,
π‘‘π‘˜
(47)
+
𝑑 ∈ (π‘‘π‘˜ , π‘‘π‘˜+1 ] , π‘˜ ∈ Z .
(i) β„Ž0 , β„Ž ∈ Γ and β„Ž0 is weakly finer than β„Ž;
(ii) there exist 𝑐 ∈ K, and function 𝑉 ∈ 𝜈0 such that
𝑉(𝑑, π‘₯) is locally Lipschtiz in π‘₯ for each 𝑑 ∈ T which is
rd, β„Ž-positive definite on 𝑆(β„Ž, 𝜌), β„Ž0 -weakly decrescent
and
𝐷+ π‘‰Δ (𝑑, π‘₯) ≤ −𝑐 (𝑉 (𝑑, π‘₯)) ,
Then, by condition (ii),
+ Δ
+
𝐷 𝐿 (𝑑, π‘₯) = 𝐷 𝑉 (𝑑, π‘₯) + 𝑐 (π‘Š (𝑑, π‘₯)) ≤ 0,
𝑑 =ΜΈ π‘‘π‘˜ ,
(48)
which implies
π‘‘π‘˜
(49)
𝑑 ∈ (π‘‘π‘˜ , π‘‘π‘˜+1 ] ,
+
for π‘˜ ∈ Z .
Hence, for πœ‰π‘–+1 ∈ (π‘‘π‘˜ , π‘‘π‘˜+1 ], we obtain, form (46), (49), and
condition (iii),
𝑉 (πœ‰π‘–+1 , π‘₯ (πœ‰π‘–+1 ))
≤
𝑉 (π‘‘π‘˜+ , π‘₯ (π‘‘π‘˜+ ))
−∫
πœ‰π‘–+1
π‘‘π‘˜
π‘‘π‘˜
𝑐 (π‘Š (𝑠, π‘₯ (𝑠))) Δ𝑠
πœ‰π‘–+1
(ii)
π‘‘π‘˜
−∫
π‘‘π‘˜−1
−∫
π‘‘π‘˜−1
𝑐 (π‘Š (𝑠, π‘₯ (𝑠))) Δ𝑠)
𝑐 (π‘Š (𝑠, π‘₯ (𝑠))) Δ𝑠
𝑑
πœ‰π‘–+1
≤ ∏ (1 + 𝑑𝑗 ) 𝑉 (𝑑0 , π‘₯0 ) − ∫
≤ 𝑀𝑉 (𝑑0 , π‘₯0 ) − 𝑐 (
(52)
If this is not true, then β„Ž0 (𝑑, π‘₯) ≥ 𝛿 for all 𝑑 ≥ 𝑑0 .
Let
≤ ⋅⋅⋅
𝑗=1
∈
Proof. By Theorem 13, system (10) is (β„Ž0 , β„Ž)-uniformly stable.
Thus, for 𝜌 > 0, there exists a 𝛿0 = 𝛿0 (𝜌) > 0 such that
β„Ž0 (𝑑0 , π‘₯0 ) < 𝛿0 implies that β„Ž(𝑑, π‘₯) < 𝜌, 𝑑 ≥ 𝑑0 , where
π‘₯(𝑑) = π‘₯(𝑑; 𝑑0 , π‘₯0 ) is any solution of (10).
Let πœ€ ∈ (0, 𝜌) be given, 𝛿 = 𝛿(πœ€) > 0 be the same as defined
in the definition of (β„Ž0 , β„Ž)-uniform stability, and β„Ž0 (𝑑0 , π‘₯0 ) <
𝛿0 . We claim that there exists a 𝑑∗ ≥ 𝑑0 such that
β„Ž0 (𝑑∗ , π‘₯ (𝑑∗ )) < 𝛿.
𝑐 (π‘Š (𝑠, π‘₯ (𝑠))) Δ𝑠
π‘˜
π‘Š(π‘‘π‘˜+ , π‘₯π‘˜ +πΌπ‘˜ (π‘₯π‘˜ ))−π‘Š(π‘‘π‘˜ , π‘₯π‘˜ ) ≤ π‘‘π‘˜ π‘Š(π‘‘π‘˜ , π‘₯π‘˜ ), (π‘‘π‘˜ , π‘₯π‘˜ )
𝑆(β„Ž, 𝜌), where π‘‘π‘˜ ≥ 0 and ∑∞
𝑖=1 𝑑𝑖 < ∞.
Then system (10) is (β„Ž0 , β„Ž)-attractive.
𝑐 (π‘Š (𝑠, π‘₯ (𝑠))) Δ𝑠
≤ (1 + π‘‘π‘˜ ) (1 + π‘‘π‘˜−1 ) 𝑉 (π‘‘π‘˜−1 , π‘₯ (π‘‘π‘˜−1 ))
πœ‰π‘–+1
0
0
+
+
π‘‘π‘˜ ) (𝑉 (π‘‘π‘˜−1
, π‘₯ (π‘‘π‘˜−1
))
πœ‰π‘–+1
(i) 𝐷+ π‘ŠΔ (𝑑, π‘₯) ≤ −𝑝(𝑑)𝑐(β„Ž0 (𝑑, π‘₯)) + π‘ž(𝑑), 𝑑 =ΜΈ π‘‘π‘˜ , (𝑑, π‘₯) ∈
∞
𝑆(β„Ž, 𝜌), where 𝑐 ∈ K, 𝑝, π‘ž ∈ πΆπ‘Ÿπ‘‘ (T, R+ ), ∫𝑑 𝑝(𝜏)Δ𝜏 =
∞
π‘‘π‘˜
−∫
Theorem 19. Assume that all conditions of Theorem 13 hold.
Suppose further, that there exists a function π‘Š ∈ 𝜈0 such that
π‘Š(𝑑, π‘₯) is locally Lipschtiz in π‘₯ for each 𝑑 ∈ T which is rd, and
the following conditions hold:
∞, and ∫𝑑 π‘ž(𝜏)Δ𝜏 < ∞;
≤ (1 + π‘‘π‘˜ ) 𝑉 (π‘‘π‘˜ , π‘₯ (π‘‘π‘˜ )) − ∫
≤ (1 +
(iii) 𝑉(π‘‘π‘˜+ , π‘₯π‘˜ + πΌπ‘˜ (π‘₯π‘˜ )) − 𝑉(π‘‘π‘˜ , π‘₯π‘˜ ) ≤ π‘‘π‘˜ 𝑉(π‘‘π‘˜ , π‘₯π‘˜ ), (π‘‘π‘˜ , π‘₯π‘˜ ) ∈
𝑆(β„Ž, 𝜌), where π‘‘π‘˜ ≥ 0 and ∑∞
𝑖=1 𝑑𝑖 < ∞.
Then system (10) is (β„Ž0 , β„Ž)-asymptotically stable.
𝑑
𝑉 (𝑑, π‘₯) ≤ 𝑉 (π‘‘π‘˜+ , π‘₯ (π‘‘π‘˜+ )) − ∫ 𝑐 (π‘Š (𝑠, π‘₯ (𝑠))) Δ𝑠,
(51)
𝑑 =ΜΈ π‘‘π‘˜ , (𝑑, π‘₯) ∈ 𝑆 (β„Ž, 𝜌) ;
Δ
𝑑0
𝐿 (𝑑, π‘₯) = π‘Š (𝑑, π‘₯) + ∫ 𝑝 (𝜏) 𝑐 (β„Ž0 (𝜏, π‘₯ (𝜏))) Δ𝜏
π‘‘π‘˜
𝑐 (π‘Š (𝑠, π‘₯ (𝑠))) Δ𝑠
𝑑
− ∫ π‘ž (𝜏) Δ𝜏,
π‘‘π‘˜
𝑏 (π‘Ÿ)
) (πœ‰π‘–+1 − 𝑑0 ) → −∞,
𝑀0
(53)
𝑑 ∈ (π‘‘π‘˜ , π‘‘π‘˜+1 ] ,
for π‘˜ ∈ Z+ . By condition (i), we obtain
𝐷+ πΏΔ (𝑑, π‘₯) = 𝐷+ π‘ŠΔ (𝑑, π‘₯) + 𝑝 (𝑑) β„Ž0 (𝑑, π‘₯) − π‘ž (𝑑)
for 𝑖 → ∞,
(50)
≤ 0,
𝑑 =ΜΈ π‘‘π‘˜ ,
(54)
8
Journal of Applied Mathematics
which implies that, for 𝑑 ∈ (π‘‘π‘˜ , π‘‘π‘˜+1 ], π‘˜ ∈ Z+ ,
𝐿 (𝑑, π‘₯) ≤ 𝐿 (π‘‘π‘˜+ , π‘₯ (π‘‘π‘˜+ )) .
(55)
Then, it follows from (55) and condition (ii) that, for 𝑑 ∈
(π‘‘π‘˜ , π‘‘π‘˜+1 ],
π‘Š (𝑑, π‘₯) ≤
π‘Š (π‘‘π‘˜+ , π‘₯ (π‘‘π‘˜+ ))
𝑑
− ∫ 𝑝 (𝜏) 𝑐 (β„Ž0 (𝜏, π‘₯ (𝜏))) Δ𝜏
π‘‘π‘˜
+ ∫ π‘ž (𝜏) Δ𝜏
(ii) there exists a constant 𝜏 > 0 such that
π‘‘π‘˜
≤ (1 + π‘‘π‘˜ ) π‘Š (π‘‘π‘˜ , π‘₯ (π‘‘π‘˜ ))
{𝑑 + π‘˜πœ : 𝑑 ∈ T, π‘˜ ∈ N} ⊂ T.
𝑑
𝑑
π‘‘π‘˜
π‘‘π‘˜
− ∫ 𝑝 (𝜏) 𝑐 (β„Ž0 (𝜏, π‘₯ (𝜏))) Δ𝜏 + ∫ π‘ž (𝜏) Δ𝜏
Proof. Since π‘Š(𝑑, π‘₯) is β„Ž0 -decrescent, there exist 𝛿1 > 0 and a
function 𝑏 ∈ K such that
+
+
× (π‘Š (π‘‘π‘˜−1
, π‘₯ (π‘‘π‘˜−1
))
π‘‘π‘˜
−∫
π‘‘π‘˜−1
+∫
π‘‘π‘˜
π‘‘π‘˜−1
π‘Š (𝑑, π‘₯) ≤ 𝑏 (β„Ž0 (𝑑, π‘₯)) ,
π‘ž (𝜏) Δ𝜏)
𝑑
𝑑
π‘‘π‘˜
π‘‘π‘˜
π‘š>
≤ (1 + π‘‘π‘˜ ) (1 + π‘‘π‘˜−1 ) π‘Š (π‘‘π‘˜−1 , π‘₯ (π‘‘π‘˜−1 ))
𝑑
π‘‘π‘˜−1
≤ ⋅⋅⋅
𝑑
𝑖=1
𝑑0
≤ ∏ (1+𝑑𝑖 ) π‘Š (𝑑0 , π‘₯0 )−∫ 𝑝 (𝜏) 𝑐 (β„Ž0 (𝜏, π‘₯ (𝜏))) Δ𝜏
π‘˜
𝑑
𝑖=2
𝑑0
(60)
π‘Š (𝑑0 + 𝑇, π‘₯ (𝑑0 + 𝑇))
≤ 𝑀0 π‘Š (𝑑0 , π‘₯0 ) − 𝑝𝑐 (𝛿) 𝑇 + 𝑀0 ∫
𝑑0 +𝑇
𝑑0
+ ∏ (1 + 𝑑𝑖 ) ∫ π‘ž (𝜏) Δ𝜏
π‘ž (𝑠) Δ𝑠
(61)
≤ 𝑀0 𝑏 (𝛿0 ) − π‘šπ‘ (𝛿) π‘πœ + 𝑀0 𝑁 < 0
𝑑
𝑑
𝑑0
𝑑0
≤ 𝑀0 (π‘Š (𝑑0 , π‘₯0 ) + ∫ π‘ž (𝜏) Δ𝜏) − 𝑐 (𝛿) ∫ 𝑝 (𝜏) Δ𝜏,
(56)
∏∞
𝑖=1 (1
where 𝑀0 =
+ 𝑑𝑖 ) < ∞. Then, (56) implies that
π‘Š(𝑑, π‘₯) → −∞, for 𝑑 → ∞. This contradiction shows that
(52) is true, and hence,
β„Ž (𝑑, π‘₯) < πœ€,
𝑀0 (𝑏 (𝛿0 ) + 𝑁)
,
π‘πœπ‘ (𝛿)
∞
π‘ž (𝜏) Δ𝜏
π‘˜
(59)
where 𝑀0 = ∏∞
π‘˜=1 (1 + π‘‘π‘˜ ) < ∞ and 𝑁 = ∫𝑑0 π‘ž(𝑠)Δ𝑠 < ∞.
Choose 𝑇 = π‘šπœ and let π‘₯(𝑑) = π‘₯(𝑑; 𝑑0 , π‘₯0 ) be any solution
of (10) with β„Ž0 (𝑑0 , π‘₯0 ) < 𝛿0 . We claim that there exists a 𝑑∗ ∈
[𝑑0 , 𝑑0 + 𝑇] such that β„Ž0 (𝑑∗ , π‘₯(𝑑∗ )) < 𝛿. If this is not true, then
β„Ž0 (𝑑, π‘₯) ≥ 𝛿 for all 𝑑∗ ∈ [𝑑0 , 𝑑0 +𝑇]. By (56), (60), and condition
(ii), we have
𝑝 (𝜏) 𝑐 (β„Ž0 (𝜏, π‘₯ (𝜏))) Δ𝜏
+ (1 + π‘‘π‘˜ ) ∫
if β„Ž0 (𝑑, π‘₯) < 𝛿1 .
By Theorem 19, system (10) is (β„Ž0 , β„Ž)-uniformly stable. Thus,
there exists a 𝛿0 = 𝛿0 (𝜌) ∈ (0, 𝛿1 ) such that β„Ž0 (𝑑0 , π‘₯0 ) < 𝛿0
implies β„Ž(𝑑, π‘₯) < 𝜌, 𝑑 ≥ 𝑑0 , for any solution π‘₯(𝑑) = π‘₯(𝑑; 𝑑0 , π‘₯0 )
of (10).
Let πœ€ ∈ (0, 𝜌) be given and 𝛿 = 𝛿(πœ€) > 0 be the same
as defined in the definition of (β„Ž0 , β„Ž)-uniformly stability. Let
π‘š > 0 be the smallest integer such that
𝑝 (𝜏) 𝑐 (β„Ž0 (𝜏, π‘₯ (𝜏))) Δ𝜏
− ∫ 𝑝 (𝜏) 𝑐 (β„Ž0 (𝜏, π‘₯ (𝜏))) Δ𝜏 + ∫ π‘ž (𝜏) Δ𝜏
π‘‘π‘˜−1
(58)
Then system (10) is uniformly asymptotically stable.
≤ (1 + π‘‘π‘˜ )
𝑑
Theorem 21. Let all the conditions of Theorem 19 and the
following additional conditions hold:
(i) π‘Š(𝑑, π‘₯) is β„Ž0 -decrescent, and 𝑝(𝑑) ≡ 𝑝 (𝑝 is a positive
constant), for 𝑑 ∈ T;
𝑑
−∫
Remark 20. When T = Z, and π‘‘π‘˜ = π‘‘π‘˜ = 0, π‘˜ ∈ N,
Theorem 19 contains Theorem 3.4 in [18] for discrete systems
without impulse effects.
Next, we will give two results on uniform asymptotic
stability in terms of two measures.
𝑑 ≥ 𝑑∗ .
Thus we conclude that system (10) is (β„Ž0 , β„Ž)-attractive.
(57)
which is a contradiction. Thus, our claim is true and by the
uniform stability we have
β„Ž (𝑑, π‘₯) < πœ€,
𝑑 ≥ 𝑑0 + 𝑇 ≥ 𝑑∗ .
(62)
Hence, system (10) is (β„Ž0 , β„Ž)-uniformly attractive. This completes the proof.
Theorem 22. Let conditions (v), (vi) of Theorem 12 hold and
assume that
(i) β„Ž0 , β„Ž ∈ Γ and β„Ž0 is finer than β„Ž;
Journal of Applied Mathematics
9
(ii) there exist a 𝑐 ∈ K, and function 𝑉 ∈ 𝜈0 such that
𝑉(𝑑, π‘₯) is locally Lipschtiz in π‘₯ for each 𝑑 ∈ T which is
rd, β„Ž-positive definite on 𝑆(β„Ž, 𝜌), β„Ž0 -decrescent and
+
Δ
𝐷 𝑉 (𝑑, π‘₯) ≤ −𝑐 (β„Ž0 (𝑑, π‘₯)) ,
𝑑 =ΜΈ π‘‘π‘˜ ,
(𝑑, π‘₯) ∈ 𝑆 (β„Ž, 𝜌) ;
which implies 𝐿(𝑑, π‘₯) ≤ 𝐿(π‘‘π‘˜+ , π‘₯(π‘‘π‘˜+ )), for 𝑑 ∈ (π‘‘π‘˜ , π‘‘π‘˜+1 ]. Then,
for 𝑑 ∈ (π‘‘π‘˜ , π‘‘π‘˜+1 ], we get
𝑑
𝑉 (𝑑, π‘₯) ≤ 𝑉 (π‘‘π‘˜+ , π‘₯ (π‘‘π‘˜+ )) − ∫ 𝑐0 (𝑠) Δ𝑠
π‘‘π‘˜
(63)
𝑑
≤ (1 + π‘‘π‘˜ ) 𝑉 (π‘‘π‘˜ , π‘₯ (π‘‘π‘˜ )) − ∫ 𝑐0 (𝑠) Δ𝑠
(iii) 𝑉(π‘‘π‘˜+ , π‘₯π‘˜ + πΌπ‘˜ (π‘₯π‘˜ )) − 𝑉(π‘‘π‘˜ , π‘₯π‘˜ ) ≤ π‘‘π‘˜ 𝑉(π‘‘π‘˜ , π‘₯π‘˜ ), (π‘‘π‘˜ , π‘₯π‘˜ ) ∈
𝑆(β„Ž, 𝜌), where π‘‘π‘˜ ≥ 0 and ∑∞
𝑖=1 𝑑𝑖 < ∞.
π‘‘π‘˜
π‘‘π‘˜
+
+
, π‘₯ (π‘‘π‘˜−1
)) − ∫
≤ (1 + π‘‘π‘˜ ) (𝑉 (π‘‘π‘˜−1
π‘‘π‘˜−1
Then system (10) is (β„Ž0 , β„Ž)-uniformly asymptotically stable.
Proof. Since 𝑉(𝑑, π‘₯) is β„Ž0 -decrescent, there exist a constant 𝛿0
and a function π‘Ž ∈ K such that
𝑉 (𝑑, π‘₯) ≤ π‘Ž (β„Ž0 (𝑑, π‘₯)) ,
if β„Ž0 (𝑑, π‘₯) < 𝛿0 .
𝑏 (β„Ž (𝑑, π‘₯)) ≤ 𝑉 (𝑑, π‘₯) ,
if β„Ž (𝑑, π‘₯) < 𝜌.
(65)
It follows from Corollary 14 that system (10) is (β„Ž0 , β„Ž)uniformly stable. Thus for 𝜌 > 0, there exist a 𝛿1 = 𝛿1 (𝜌) ∈
(0, 𝛿0 ) such that β„Ž0 (𝑑0 , π‘₯0 ) < 𝛿1 implies
𝑑 ≥ 𝑑0 .
β„Ž (𝑑, π‘₯) < 𝜌,
𝑑
− ∫ 𝑐0 (𝑠) Δ𝑠
π‘‘π‘˜
(66)
(72)
+
+
≤ (1 + π‘‘π‘˜ ) (1 + π‘‘π‘˜−1 ) 𝑉 (π‘‘π‘˜−1
, π‘₯ (π‘‘π‘˜−1
))
(64)
The fact that 𝑉(𝑑, π‘₯) is β„Ž-positive definite on 𝑆(β„Ž, 𝜌) implies
that there exists a function 𝑏 ∈ K such that
−∫
𝑑
π‘‘π‘˜−1
𝑐0 (𝑠) Δ𝑠
π‘˜
𝑑
𝑖=1
𝑑0
≤ 𝑉 (𝑑0 , π‘₯0 ) ∏ (1 + 𝑑𝑖 ) − ∫ 𝑐0 (𝑠) Δ𝑠
𝑑
≤ 𝑀𝑉 (𝑑0 , π‘₯0 ) − ∫ 𝑐0 (𝑠) Δ𝑠,
𝑑0
where 𝑐0 (𝑑) := 𝑐(β„Ž0 (𝑑, π‘₯)). Hence, for 𝑑 = 𝑑0 + 𝑇, we obtain
𝑉(𝑑, π‘₯(𝑑))|𝑑=𝑑0 +𝑇 ≤ 𝑀𝑉 (𝑑0 , π‘₯0 ) − ∫
By the choice of 𝛿1 , we get
𝑑0 +𝑇
𝑑0
𝑉 (𝑑0 , π‘₯0 ) ≤ π‘Ž (β„Ž0 (𝑑0 , π‘₯0 )) ≤ π‘Ž (𝛿1 ) .
(67)
To prove the theorem, it is enough to show that system
(10) is (β„Ž0 , β„Ž)-uniformly attractive.
Given 0 < πœ€ < 𝜌, let 𝛿 = 𝛿(πœ€) > 0 be the same as defined
in the definition of (β„Ž0 , β„Ž)-uniformly stability. Then for any
solution π‘₯(𝑑) = π‘₯(𝑑; 𝑑0 , π‘₯0 ) of system (10) with β„Ž0 (𝑑0 , π‘₯0 ) < 𝛿1 ,
we claim that there exists a 𝑇 = 𝑇(πœ€) > π‘€π‘Ž(𝛿1 )/𝑐(𝛿) such
that, for some 𝑑∗ ∈ [𝑑0 , 𝑑0 + 𝑇],
β„Ž0 (𝑑∗ , π‘₯ (𝑑∗ )) < 𝛿,
(68)
where 𝑀 = ∏∞
π‘˜=1 (1 + π‘‘π‘˜ ) < ∞. Suppose that this is false.
Then for any 𝑇 > π‘€π‘Ž(𝛿1 )/𝑐(𝛿) there exists a solution π‘₯(𝑑) =
π‘₯(𝑑; 𝑑0 , π‘₯0 ) of (10) satisfying β„Ž0 (𝑑0 , π‘₯0 ) < 𝛿1 , such that
β„Ž0 (𝑑, π‘₯ (𝑑)) ≥ 𝛿,
𝑑 ∈ [𝑑0 , 𝑑0 + 𝑇] .
(69)
By setting
𝑑
𝐿 (𝑑, π‘₯) = 𝑉 (𝑑, π‘₯) + ∫ 𝑐 (β„Ž0 (𝑠, π‘₯ (𝑠))) Δ𝑠,
π‘‘π‘˜
(70)
𝑑 ∈ (π‘‘π‘˜ , π‘‘π‘˜+1 ] , π‘˜ ∈ Z ,
𝑐 (β„Ž0 (𝑠, π‘₯ (𝑠))) Δ𝑠
≤ π‘€π‘Ž (𝛿1 ) − 𝑐 (𝛿) 𝑇 < 0
(73)
which is a contradiction. Hence there exists a number 𝑑∗ ∈
(𝑑0 , 𝑑0 + 𝑇] such that β„Ž0 (𝑑∗ , π‘₯(𝑑∗ )) < 𝛿. Then for 𝑑 ≥ 𝑑∗ , thus
for 𝑑 ≥ 𝑑0 + 𝑇 as well, we have
β„Ž (𝑑, π‘₯) < πœ€,
(74)
that is, β„Ž(𝑑, π‘₯) < πœ€ holds for 𝑑 ≥ 𝑑0 +𝑇 which means that system
(10) is uniformly attractive. Theorem 22 is proved.
4.3. (β„Ž0 ,β„Ž)-Instability
Theorem 23. Assume that
(i) β„Ž0 , β„Ž ∈ Γ, 𝑉 ∈ 𝜈0 , 𝑉(𝑑, π‘₯) is locally Lipschtiz in π‘₯ for
each 𝑑 ∈ T which is rd, β„Ž-positive definite on 𝑆(β„Ž, 𝜌),
and
𝐷+ π‘‰Δ (𝑑, π‘₯) ≥ 0,
+
𝑐0 (𝑠) Δ𝑠)
𝑑 =ΜΈ π‘‘π‘˜ , (𝑑, π‘₯) ∈ 𝑆 (β„Ž, 𝜌) ,
(75)
and for any 𝑠 ≥ 𝑑0 and 𝛼 > 0, there is 𝛽 > 0 such that
𝑉(𝑑, π‘₯) ≥ 𝛼 for 𝑑 ≥ 𝑠 implies β„Ž(𝑑, π‘₯) ≥ 𝛽 for 𝑑 ≥ 𝑠;
(ii) for (π‘‘π‘˜ , π‘₯π‘˜ ) ∈ 𝑆(β„Ž, 𝜌), π‘˜ ∈ N,
and condition (ii), we have
𝐷+ πΏΔ (𝑑, π‘₯) = 𝐷+ π‘‰Δ (𝑑, π‘₯) + 𝑐 (β„Ž0 (𝑑, π‘₯)) ≤ 0,
𝑑 =ΜΈ π‘‘π‘˜ ,
(71)
𝑉 (π‘‘π‘˜+ , π‘₯ (π‘‘π‘˜+ )) − 𝑉 (π‘‘π‘˜ , π‘₯π‘˜ )
≥ πœ† π‘˜ πœ“ (𝑉 (π‘‘π‘˜ , π‘₯π‘˜ )) ,
(76)
10
Journal of Applied Mathematics
+
where πœ† π‘˜ ≥ 0 with ∑∞
→ R+ is
π‘˜=1 πœ† π‘˜ = ∞, πœ“ : R
nondecreasing and πœ“(0) = 0, πœ“(𝑠) > 0 for 𝑠 > 0.
(iii) for any 𝑒 > 0,
−∫
Then system (10) is (β„Ž0 , β„Ž)-unstable.
π‘‘π‘˜
Proof. Let us assume on the contrary that system (10) is
(β„Ž0 , β„Ž)-stable. Then for 0 < πœ€ < 𝜌, there exists a 𝛿 = 𝛿(𝑑0 , πœ€) >
0 such that β„Ž0 (𝑑0 , π‘₯0 ) < 𝛿 implies that β„Ž(𝑑, π‘₯) < πœ€ for 𝑑 ≥ 𝑑0 .
By setting 𝐿(𝑑) = 𝑉(𝑑, π‘₯), we know from condition (i) and
(ii) that 𝐿(𝑑) is right-nondecreasing for 𝑑 ≥ 𝑑0 . Then, 𝐿(𝑑) ≥
𝐿(𝑑0 ), if 𝑑 ≥ 𝑑0 . Thus, it follows from condition (i) that there
exists a 𝛽0 = 𝛽0 (𝐿(𝑑0 )) > 0 such that β„Ž(𝑑, π‘₯) ≥ 𝛽0 for 𝑑 ≥ 𝑑0 .
Since 𝑉(𝑑, π‘₯) is β„Ž-positive definite on 𝑆(β„Ž, 𝜌), there exists 𝑏 ∈
K such that 𝑏(β„Ž(𝑑, π‘₯)) ≤ 𝑉(𝑑, π‘₯), if β„Ž(𝑑, π‘₯) < 𝜌. Then, we have
𝐿 (π‘‘π‘˜ ) ≥ 𝑏 (β„Ž (π‘‘π‘˜ , π‘₯π‘˜ )) ≥ 𝑏 (𝛽0 ) ,
π‘‘π‘˜+1
π‘˜ ∈ N.
(77)
From condition (ii) and (77), we have
+
𝐿 (π‘‘π‘˜+ ) − 𝐿 (π‘‘π‘˜−1
) ≥ 𝐿 (π‘‘π‘˜+ ) − 𝐿 (π‘‘π‘˜ )
≥ πœ† π‘˜ πœ“ (𝐿 (π‘‘π‘˜ )) ≥ πœ† π‘˜ πœ“ (𝑏 (𝛽0 )) ,
(78)
𝑔 (𝜏) Δ𝜏 +
πœ“π‘˜ (𝑒) − 𝑒
≥ π‘Ÿπ‘˜ ,
𝑐 (𝑒)
π‘˜ ∈ N,
(82)
where π‘Ÿπ‘˜ ≥ 0 and ∑∞
𝑖=1 π‘Ÿπ‘˜ = ∞.
Then system (10) is (β„Ž0 , β„Ž)-unstable.
Proof. For the sake of contradiction, we assume that system
(10) is (β„Ž0 , β„Ž)-stable. Then for 0 < πœ€ < 𝜌, there exists a 𝛿 =
𝛿(𝑑0 , πœ€) > 0 such that β„Ž0 (𝑑0 , π‘₯0 ) < 𝛿 implies β„Ž(𝑑, π‘₯) < πœ€ for
𝑑 ≥ 𝑑0 . Since 𝑉(𝑑, π‘₯) is β„Ž-decrescent on 𝑆(β„Ž, 𝜌), there exists a
function π‘Ž ∈ K such that
𝑉 (𝑑, π‘₯) ≤ π‘Ž (β„Ž (𝑑, π‘₯)) < π‘Ž (𝜌) ,
if β„Ž (𝑑, π‘₯) < 𝜌.
(83)
Let π‘š(t)
=
𝑉(𝑑, π‘₯) and 𝐿(𝑑)
=
𝑉(𝑑, π‘₯) +
𝑑
∫𝑑 𝑔(𝜏)𝑐(𝑉(𝜏, π‘₯(𝜏)))Δ𝜏, for 𝑑 ∈ (π‘‘π‘˜ , π‘‘π‘˜+1 ], π‘˜ ∈ Z+ . Then
π‘˜
it follows from condition (i) that
𝐷+ πΏΔ (𝑑) = 𝐷+ π‘‰Δ (𝑑, π‘₯) + 𝑔 (𝑑) 𝑐 (𝑉 (𝑑, π‘₯)) ≥ 0,
𝑑 =ΜΈ π‘‘π‘˜ ,
(84)
which implies
and so
𝐿 (π‘‘π‘˜+ )
≥
+
𝐿 (π‘‘π‘˜−1
)
𝐿 (𝑑) ≥ 𝐿 (π‘‘π‘˜+ ) ,
+ πœ† π‘˜ πœ“ (𝑏 (𝛽0 ))
π‘š (π‘‘π‘˜+1 ) − π‘š (π‘‘π‘˜+ ) ≥ − ∫
π‘‘π‘˜+1
π‘‘π‘˜
≥ ⋅⋅⋅
≥ 𝐿 (𝑑1 ) + πœ“ (𝑏 (𝛽0 )) ∑πœ† 𝑖 → ∞,
≥
as π‘˜ → ∞,
𝑖=1
(79)
which implies that, for a given number 𝑀 ≫ 0, there exists
a 𝑠 ≥ 𝑑0 such that 𝐿(𝑑) ≥ 𝑀 for 𝑑 ≥ 𝑠. Thus by condition (i),
there is a 𝛽 = 𝛽(𝑀) > 0 such that β„Ž(𝑑, π‘₯) ≥ 𝛽 for 𝑑 ≥ 𝑠 which is
a contradiction to the (β„Ž0 , β„Ž)-stability. Therefore, system (10)
is (β„Ž0 , β„Ž)-unstable.
𝑑 =ΜΈ π‘‘π‘˜ , (𝑑, π‘₯) ∈ 𝑆 (β„Ž, 𝜌) ,
(86)
𝑔 (𝜏) Δ𝜏.
≥ πœ“π‘˜ (π‘š (π‘‘π‘˜+ )) − π‘š (π‘‘π‘˜+ )
(87)
which, together with (86) and condition (iii), yields
π‘š (π‘‘π‘˜+1 ) − π‘š (π‘‘π‘˜ ) = π‘š (π‘‘π‘˜+1 ) − π‘š (π‘‘π‘˜+ ) + π‘š (π‘‘π‘˜+ ) − π‘š (π‘‘π‘˜ )
≥ πœ“π‘˜ (π‘š (π‘‘π‘˜+ )) − π‘š (π‘‘π‘˜+ )
− 𝑐 (π‘š (π‘‘π‘˜+ )) ∫
π‘‘π‘˜+1
π‘‘π‘˜
𝑔 (𝜏) Δ𝜏
≥ 𝑐 (π‘š (π‘‘π‘˜+ )) π‘Ÿπ‘˜ ≥ 𝑐 (π‘š (π‘‘π‘˜ )) π‘Ÿπ‘˜
(80)
≥ 𝑐 (π‘š (𝑑1 )) π‘Ÿπ‘˜ ,
π‘˜ ∈ N.
(88)
Thus,
where 𝑔 ∈ πΆπ‘Ÿπ‘‘ (T, R+ ) and 𝑐 ∈ K;
(ii) there exist πœ“π‘˜ : R+ → R+ , π‘˜ ∈ N, such that πœ“π‘˜ (𝑠) > 𝑠,
πœ“π‘˜ (𝑠) − 𝑠 ≥ πœ“π‘˜ (𝑑) − 𝑑 for 𝑑 ≥ 𝑠 ≥ 0, and
𝑉 (π‘‘π‘˜+ , π‘₯π‘˜ + πΌπ‘˜ (π‘₯π‘˜ )) ≥ πœ“π‘˜ (𝑉 (π‘‘π‘˜ , π‘₯π‘˜ )) ,
π‘‘π‘˜+1
−𝑐 (π‘š (π‘‘π‘˜+ )) ∫
π‘‘π‘˜
π‘š (π‘‘π‘˜+ ) − π‘š (π‘‘π‘˜ ) ≥ πœ“π‘˜ (π‘š (π‘‘π‘˜ )) − π‘š (π‘‘π‘˜ )
(i) β„Ž0 , β„Ž ∈ Γ, 𝑉 ∈ 𝜈0 , 𝑉(𝑑, π‘₯) is locally Lipschtiz in π‘₯ for
each 𝑑 ∈ T which is rd, β„Ž-decrescent on 𝑆(β„Ž, 𝜌), and
−𝑔 (𝑑) 𝑐 (𝑉 (𝑑, π‘₯)) ≤ 𝐷+ π‘‰Δ (𝑑, π‘₯) ≤ 0,
𝑔 (𝜏) 𝑐 (π‘š (𝜏)) Δ𝜏
From condition (ii), we have
Theorem 24. Assume that
(π‘‘π‘˜ , π‘₯π‘˜ ) ∈ 𝑆 (β„Ž, 𝜌) , π‘˜ ∈ N;
(85)
Since 𝐷+ π‘‰Δ (𝑑, π‘₯) ≤ 0, it follows from (85), that
+
) + (πœ† π‘˜−1 + πœ† π‘˜ ) πœ“ (𝑏 (𝛽0 ))
≥ 𝐿 (π‘‘π‘˜−2
π‘˜
𝑑 ∈ (π‘‘π‘˜ , π‘‘π‘˜+1 ] .
π‘˜
π‘š (π‘‘π‘˜+1 ) ≥ π‘š (𝑑1 ) + 𝑐 (π‘š (𝑑1 )) ∑π‘Ÿπ‘– 󳨀→ ∞,
as π‘˜ 󳨀→ ∞,
𝑖=1
(89)
(81)
which contradicts (83). Therefore, system (10) is (β„Ž0 , β„Ž)unstable and the proof is complete.
Journal of Applied Mathematics
11
where π‘₯𝜎 (𝑑) = π‘₯(𝜎(𝑑)), and
5. Examples
In this section, as applications of the above-derived theoretical criteria, two representative examples are given as follows.
Example 25. Consider the system
𝑉 (π‘₯ (π‘‘π‘˜+ ) , 𝑦 (π‘‘π‘˜+ ))
= π‘₯2 (π‘‘π‘˜+ ) + 𝑦2 (π‘‘π‘˜+ )
= (1 +
π‘₯Δ (𝑑) =
𝑦 (𝑑)
− π‘₯ (𝑑) ,
2 (1 + π‘₯2 (𝑑))
𝑑 =ΜΈ π‘‘π‘˜ ,
π‘¦Δ (𝑑) =
π‘₯ (𝑑)
− 𝑦 (𝑑) ,
2 (1 + 𝑦2 (𝑑))
𝑑 =ΜΈ π‘‘π‘˜ ,
≤ 𝑉 (π‘₯ (π‘‘π‘˜ ) , 𝑦 (π‘‘π‘˜ )) +
(90)
𝑉 (π‘₯ (π‘‘π‘˜+ ) , 𝑦 (π‘‘π‘˜+ )) − 𝑉 (π‘₯ (π‘‘π‘˜ ) , 𝑦 (π‘‘π‘˜ )) ≤ π‘‘π‘˜ 𝑉 (π‘₯ (π‘‘π‘˜ ) , 𝑦 (π‘‘π‘˜ )) ,
(93)
Δ𝑦 (π‘‘π‘˜ ) =
5
𝑦 (π‘‘π‘˜ ) ,
2π‘˜
π‘˜ ∈ N,
where π‘‘π‘˜ = 1/2π‘˜−5 and ∏∞
π‘˜=1 π‘‘π‘˜ < ∞.
If πœ‡(𝑑) ≤ 2, then by (91) we have
π‘‰Δ (π‘₯, 𝑦) ≤ 0.
(94)
Then for β„Ž(π‘₯, 𝑦) = |π‘₯| and β„Ž0 (π‘₯, 𝑦) = √π‘₯2 + 𝑦2 , we have
= π‘₯ Δ π‘₯ + π‘₯ 𝜎 π‘₯ Δ + 𝑦 Δ π‘¦ + 𝑦 𝜎 𝑦Δ
= π‘₯Δ (2π‘₯ + πœ‡π‘₯Δ ) + π‘¦Δ (2𝑦 + πœ‡π‘¦Δ )
π‘‰Δ (π‘₯, 𝑦) ≤ −π‘šπ‘‰ (π‘₯, 𝑦) .
𝑦
π‘₯
− π‘₯) + 2𝑦 (
− 𝑦)
2
2 (1 + π‘₯ )
2 (1 + 𝑦2 )
+ πœ‡ [(
2
𝑦
π‘₯
− π‘₯) + (
− 𝑦) ]
2
2(1 + π‘₯ )
2(1 + 𝑦2 )
2
(1 + π‘₯2 )
β„Ž (π‘₯, 𝑦) ≤ 𝑉 (π‘₯, 𝑦) ≤ β„Ž0 (π‘₯, 𝑦) .
+ (πœ‡ − 2) (π‘₯2 + 𝑦2 )
(1 − πœ‡) π‘₯𝑦 (1 + 𝑦2 ) + (πœ‡/4) π‘₯2
(1/2) (1 − πœ‡) (π‘₯2 + 𝑦2 ) (1 + π‘₯2 ) + (πœ‡/4) (π‘₯2 + 𝑦2 )
2
π‘₯2 )
+ (πœ‡ − 2) (π‘₯2 + 𝑦2 )
2
2
2
2
2
(1/2) (1 − πœ‡) (π‘₯ + 𝑦 ) (1 + 𝑦 ) + (πœ‡/4) (π‘₯ + 𝑦 )
1
≤ (πœ‡ − 2) 𝑉 (π‘₯, 𝑦) ,
2
(1 +
(97)
By Corollary 18, we conclude that system (90) is (β„Ž0 , β„Ž)asymptotically stable. Moreover, since β„Ž0 = 𝑉, we conclude,
by Theorem 22, that system (90) is (β„Ž0 , β„Ž)-uniformly asymptotically stable.
Example 26. Consider the following system [14]
2
(1 + 𝑦2 )
(1 +
(96)
Then for β„Ž(π‘₯, 𝑦) = 2|π‘₯𝑦| and β„Ž0 (π‘₯, 𝑦) = π‘₯2 + 𝑦2 , we have
2
(1 − πœ‡) π‘₯𝑦 (1 + π‘₯2 ) + (πœ‡/4) 𝑦2
(95)
From Corollary 14, we conclude that system (90) is (β„Ž0 , β„Ž)uniformly stable. It should be noted that (β„Ž0 , β„Ž)-stability in
this case implies, by the choice of β„Ž and β„Ž0 , that the trivial
solution of (90) is partially stable with respect to π‘₯.
If, for a given positive constant π‘š ≤ 1, πœ‡(𝑑) ≤ 2(1 − π‘š),
then we have
2 Δ
= (π‘₯ + 𝑦 )
+
that is,
β„Ž2 (π‘₯, 𝑦) ≤ 𝑉 (𝑑, π‘₯) ≤ β„Ž02 (π‘₯, 𝑦) .
2
≤
(92)
π‘˜ ∈ N,
π‘‰Δ (π‘₯, 𝑦)
+
π‘˜ ∈ N,
3
π‘₯ (π‘‘π‘˜ ) ,
2π‘˜
Let 𝑉(π‘₯, 𝑦) = π‘₯2 + 𝑦2 . Then we have
=
1
𝑉 (π‘₯ (π‘‘π‘˜ ) , 𝑦 (π‘‘π‘˜ )) ,
2π‘˜−5
Δπ‘₯ (π‘‘π‘˜ ) =
on time scale T.
= 2π‘₯ (
5 2
3 2 2
) π‘₯ (π‘‘π‘˜ ) + (1 + π‘˜ ) 𝑦2 (π‘‘π‘˜ )
π‘˜
2
2
2
𝑦2 )
𝑑 =ΜΈ π‘‘π‘˜ ,
(91)
π‘₯1Δ = − (𝑒−𝑑 + 1) π‘₯1 −
π‘₯1 π‘₯22
,
1 + π‘₯22
𝑑 =ΜΈ π‘‘π‘˜ ,
π‘₯2Δ = − (𝑒−𝑑 + 1) π‘₯2 −
π‘₯12 π‘₯2
,
1 + π‘₯12
𝑑 =ΜΈ π‘‘π‘˜ ,
1
Δπ‘₯1 = π‘₯1 ,
2
𝑑 = π‘‘π‘˜ , π‘˜ ∈ N,
1
Δπ‘₯2 = π‘₯2 ,
2
𝑑 = π‘‘π‘˜ , π‘˜ ∈ N,
on time scale T such that πœ‡(𝑑) ≥ 2/(𝑒−𝑑 + 1), for all 𝑑 ∈ T.
(98)
12
Journal of Applied Mathematics
Let 𝑉(𝑑, π‘₯) = π‘₯12 + π‘₯22 , then we get
π‘‰Δ (𝑑, π‘₯) = π‘₯1Δ π‘₯1 + π‘₯1𝜎 π‘₯1Δ + π‘₯2Δ π‘₯2 + π‘₯2𝜎 π‘₯2Δ
= π‘₯1Δ π‘₯1 + (π‘₯1 + πœ‡π‘₯1𝜎 ) π‘₯1Δ + π‘₯2Δ π‘₯2 + (π‘₯2 + πœ‡π‘₯2𝜎 ) π‘₯2Δ
2
2
= 2π‘₯1Δ π‘₯1 + 2π‘₯2Δ π‘₯2 + πœ‡ [(π‘₯1Δ ) + (π‘₯2Δ ) ] ,
(99)
where π‘₯π‘–πœŽ = π‘₯𝑖 (𝜎(𝑑)), 𝑖 = 1, 2. Substituting (98) into (99) yields
2
π‘‰Δ (𝑑, π‘₯) = [πœ‡ (𝑒−𝑑 + 1) − 2 (𝑒−𝑑 + 1)] (π‘₯12 + π‘₯22 )
+
πœ‡π‘₯12 π‘₯24
(1 +
2
π‘₯22 )
+
πœ‡π‘₯14 π‘₯22
(1 + π‘₯12 )
+ 2 [πœ‡ (𝑒−𝑑 + 1) − 1] (
≥
π‘₯12 π‘₯24
(1 +
2
π‘₯22 )
+
π‘₯14 π‘₯22
2
(1 + π‘₯12 )
2
π‘₯12 π‘₯22
π‘₯12 π‘₯22
+
)
1 + π‘₯12 1 + π‘₯22
≥ 0.
(100)
When 𝑑 = π‘‘π‘˜ , we have
9
9
𝑉 (π‘‘π‘˜+ , π‘₯ (π‘‘π‘˜+ )) = π‘₯12 (π‘‘π‘˜+ ) + π‘₯22 (π‘‘π‘˜+ ) = π‘₯12 (π‘‘π‘˜ ) + π‘₯22 (π‘‘π‘˜ )
4
4
= 𝑉 (π‘‘π‘˜ , π‘₯ (π‘‘π‘˜ )) + πœ† π‘˜ πœ“ (𝑉 (π‘‘π‘˜ , π‘₯ (π‘‘π‘˜ ))) ,
(101)
where πœ† π‘˜ ≡ 5/4 and πœ“(𝑠) = 𝑠.
For β„Ž(𝑑, π‘₯) = |π‘₯1 | + |π‘₯2 | and β„Ž0 ∈ Γ, we have
󡄨 󡄨 󡄨 󡄨2
β„Ž2 (𝑑, π‘₯) = (󡄨󡄨󡄨π‘₯1 󡄨󡄨󡄨 + 󡄨󡄨󡄨π‘₯2 󡄨󡄨󡄨) = π‘₯12 + π‘₯22 + 2π‘₯1 π‘₯2 ≥ 𝑉 (𝑑, π‘₯) .
(102)
Then, for any 𝑠 ≥ 𝑑0 and 𝛼 > 0, 𝑉(𝑑, π‘₯) ≥ 𝛼 implies that
β„Ž(𝑑, π‘₯) ≥ 𝛽 = √𝛼. Hence, all the conditions of Theorem 23
are satisfied, and system (98) is (β„Ž0 , β„Ž)-unstable.
6. Conclusions
We have generalized the concepts of stability in terms of
two measures relative to ordinary impulsive systems to
impulsive systems on time scales. By employing the approach
of Lyapunov function, we have established some criteria
ensuring stability and instability in terms of two measures
for nonlinear impulsive systems on time scales. Two examples
have been worked out to demonstrate the main results.
References
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[3] X. Liu and G. Ballinger, “Boundedness for impulsive delay
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