time delay and mean square stochastic differential equations in impetuous stabilization

5
@ IJTSRD | Available Online @ www ISSN No: 245 Inte R Time Delay and Mean in I G. Pramila Department of Mathematic Vivekanandha College of Arts and S Women (Autonomous), Elayamp Thiruchengode, Namakkal, Tamil N ABSTRACT This paper specially exhibits about the t mean square stochastic differential impetuous stabilization is analyzed. By delay differential inequality and using analysis technique, a few present sta square exponential stabilization are s express that an unstable stochastic dela be achieved some stability by imp example is also argued to derived the ef obtained results. Keywords: Impetuous stabilization, stochastic delay differential equation inequality 1. INTRODUCTION Impetuous control and stability has bee the variety of areas has found many app studied over the past centuries, such as o of satellite [11], ecosystems manage dosage supply in pharmacokinetics [14] and synchronization in chaotic secure c systems and other chaotic systems [15,1 many significant results for the impetuo stabilization of delay differential system Systematically, the input states of syst get the disturbance of delay phenomena the disturbance of mean square stochast in many practical problems. In curre stability investigation of impetuous sto differential systems is catching to many w.ijtsrd.com | Volume – 2 | Issue – 3 | Mar-Apr 56 - 6470 | www.ijtsrd.com | Volum ernational Journal of Trend in Sc Research and Development (IJT International Open Access Journ n Square Stochastic Differentia Impetuous Stabilization cs, Sciences for palayam, Nadu, India S. Ramad Department of M Vivekanandha College of A Women (Autonomous), Thiruchengode, Namakka time delay and equations in y projecting a the stochastic age for mean survived. It is ay system can petuous. This fficiency of the mean square n, differential en extensively plication to be orbital transfer ement [12,13], ], and stability communication 16]. At present, ous control and ms. tems not only a, but also get tic phenomena ent years, the ochastic delay authors, and a large number of stability cr have been reported [1-6]. How all needed so that the corre stochastic delay different impetuous must be stable itsel impetuous are only to inhibi square stochastic delay Although, it is known that the guiding how a proper Lyapu constructed for a given mode impetuous to projecting a new the impetuous stabilization of functional differential equatio the Lyapunov functional. Without motivation from the main aim in this paper is to t and mean square stochastic d impetuous stabilization. By differential inequality and analysis technique, some su mean square exponential stabi 2. Model and Preliminaries In this paper, unless otherwise standard notation used previou denote the n-dimensional uni Euclidean norm, β‰œ {1,2, … , }, β„• β‰œ {1,2, … (0, ∞). for ∈ ℝ Γ— , ΰ―« r 2018 Page: 627 me - 2 | Issue – 3 cientific TSRD) nal al Equations devi Mathematics, Arts and Sciences for , Elayampalayam, al, Tamil Nadu, India riteria of these systems wever, these criteria are esponding mean square tial systems without lf, which implies that the it the stability of mean differential systems. er is no general rule for unov functional can be el. Therefore, it is very w approach to studying f mean square stochastic ons without resorting to above discussions, our the study the time delay differential equations in y projecting a delay using the stochastic ufficient conditions for ility are obtained. e specified, we adopt the usly by Yang [8]. Let E it matrix, |. | denote the }, ℝ ΰ¬Ύ = [0, ∞), ℝ ΰ¬Ύ = ΰ―« () () are

Upload: ijtsrd

Post on 13-Aug-2019

11 views

Category:

Education


2 download

DESCRIPTION

This paper specially exhibits about the time delay and mean square stochastic differential equations in impetuous stabilization is analyzed. By projecting a delay differential inequality and using the stochastic analysis technique, a few present stage for mean square exponential stabilization are survived. It is express that an unstable stochastic delay system can be achieved some stability by impetuous. This example is also argued to derived the efficiency of the obtained results. G. Pramila | S. Ramadevi "Time Delay and Mean Square Stochastic Differential Equations in Impetuous Stabilization" Published in International Journal of Trend in Scientific Research and Development (ijtsrd), ISSN: 2456-6470, Volume-2 | Issue-3 , April 2018, URL: https://www.ijtsrd.com/papers/ijtsrd11062.pdf Paper URL: http://www.ijtsrd.com/humanities-and-the-arts/other/11062/time-delay-and-mean-square-stochastic-differential-equations-in-impetuous-stabilization/g-pramila

TRANSCRIPT

Page 1: Time Delay and Mean Square Stochastic Differential Equations in Impetuous Stabilization

@ IJTSRD | Available Online @ www.ijtsrd.com

ISSN No: 2456

InternationalResearch

Time Delay and Mean Square Stin Impetuous Stabilization

G. Pramila Department of Mathematics,

Vivekanandha College of Arts and Sciences for Women (Autonomous), Elayampalayam,

Thiruchengode, Namakkal, Tamil Nadu, India

ABSTRACT This paper specially exhibits about the time delay and mean square stochastic differential equations in impetuous stabilization is analyzed. By projecting a delay differential inequality and using the stochastic analysis technique, a few present stage for mean square exponential stabilization are survived. It is express that an unstable stochastic delay system can be achieved some stability by impetuous. This example is also argued to derived the efficiency of the obtained results.

Keywords: Impetuous stabilization, mean square stochastic delay differential equation, differential inequality

1. INTRODUCTION

Impetuous control and stability has been extensively the variety of areas has found many application to be studied over the past centuries, such as orbital transfer of satellite [11], ecosystems management [12,13], dosage supply in pharmacokinetics [14], and stability and synchronization in chaotic secure commsystems and other chaotic systems [15,16]. At present, many significant results for the impetuousstabilization of delay differential systems.

Systematically, the input states of systems not only get the disturbance of delay phenomena, but also the disturbance of mean square stochastic phenomena in many practical problems. In current years, the stability investigation of impetuous stochastic delay differential systems is catching to many authors, and a

@ IJTSRD | Available Online @ www.ijtsrd.com | Volume – 2 | Issue – 3 | Mar-Apr 2018

ISSN No: 2456 - 6470 | www.ijtsrd.com | Volume

International Journal of Trend in Scientific Research and Development (IJTSRD)

International Open Access Journal

nd Mean Square Stochastic Differential Equationsn Impetuous Stabilization

Department of Mathematics, Vivekanandha College of Arts and Sciences for

yampalayam, , Namakkal, Tamil Nadu, India

S. RamadeviDepartment of Mathematics,

Vivekanandha College of Arts and Sciences for Women (Autonomous),

Thiruchengode, Namakkal, Tamil Nadu, India

This paper specially exhibits about the time delay and mean square stochastic differential equations in impetuous stabilization is analyzed. By projecting a

using the stochastic analysis technique, a few present stage for mean square exponential stabilization are survived. It is express that an unstable stochastic delay system can be achieved some stability by impetuous. This

the efficiency of the

Impetuous stabilization, mean square stochastic delay differential equation, differential

tability has been extensively the variety of areas has found many application to be

, such as orbital transfer , ecosystems management [12,13],

dosage supply in pharmacokinetics [14], and stability and synchronization in chaotic secure communication systems and other chaotic systems [15,16]. At present,

esults for the impetuous control and systems.

Systematically, the input states of systems not only get the disturbance of delay phenomena, but also get

stochastic phenomena current years, the

investigation of impetuous stochastic delay to many authors, and a

large number of stability criteria of these systems have been reported [1-6]. However, these criteria are all needed so that the correspondingstochastic delay differential systems impetuous must be stable itself, which implies that the impetuous are only to inhibit the stability of square stochastic delay differential systems. Although, it is known that ther is no general rule for guiding how a proper Lyapunov functional can be constructed for a given model.impetuous to projecting a new approach to studying the impetuous stabilization of mean square stochastic functional differential equations without resorting to the Lyapunov functional.

Without motivation from the above discussions, our main aim in this paper is to the study the time delay and mean square stochastic differential eqimpetuous stabilization. By projecting a delaydifferential inequality and using the stochastic analysis technique, some sufficient conditions for mean square exponential stability are obtained.

2. Model and Preliminaries

In this paper, unless otherwise specified, we adopt the standard notation used previously by Yang [8]. Let E denote the n-dimensional unit matrix, Euclidean norm,

𝒩 β‰œ {1,2, … , 𝑛}, β„• β‰œ {1,2, …(0, ∞). for 𝐴 ∈ ℝ Γ— , πœ†

Apr 2018 Page: 627

6470 | www.ijtsrd.com | Volume - 2 | Issue – 3

Scientific (IJTSRD)

International Open Access Journal

tial Equations

Ramadevi Department of Mathematics,

Vivekanandha College of Arts and Sciences for Women (Autonomous), Elayampalayam,

, Namakkal, Tamil Nadu, India

large number of stability criteria of these systems ]. However, these criteria are

all needed so that the corresponding mean square stochastic delay differential systems without impetuous must be stable itself, which implies that the impetuous are only to inhibit the stability of mean

y differential systems. , it is known that ther is no general rule for

guiding how a proper Lyapunov functional can be n model. Therefore, it is very

impetuous to projecting a new approach to studying on of mean square stochastic

functional differential equations without resorting to

Without motivation from the above discussions, our main aim in this paper is to the study the time delay and mean square stochastic differential equations in impetuous stabilization. By projecting a delay differential inequality and using the stochastic analysis technique, some sufficient conditions for mean square exponential stability are obtained.

In this paper, unless otherwise specified, we adopt the standard notation used previously by Yang [8]. Let E

dimensional unit matrix, |. | denote the

}, ℝ = [0, ∞), ℝ =(𝐴)π‘Žπ‘›π‘‘ πœ† (𝐴) are

Page 2: Time Delay and Mean Square Stochastic Differential Equations in Impetuous Stabilization

International Journal of Trend in Scientific Research and Development (IJTSRD) ISSN: 2456-6470

@ IJTSRD | Available Online @ www.ijtsrd.com | Volume – 2 | Issue – 3 | Mar-Apr 2018 Page: 628

largest and smallest singular values of A, respectively. ‖𝐴‖ = πœ† (𝐴 𝐴).

B[X,Y] denotes the space of continuous mappings from the topological space Y. In particular, let 𝐡 β‰œ 𝐡[[βˆ’πœ, 0], ℝ ], where 𝜏 > 0:

PB[𝕁, ℝ ] = {ψ: 𝕁 β†’ ℝ ∣ψ(s)is continuous for all but at most countable ponit s ∈ 𝕁 and at these points βˆˆπ•, ψ(s )andψ(s ) exist and ψ(s) = ψ(s )},

Where 𝕁 βŠ‚ ℝ is an interval, ψ(s )andψ(s ) denot the right-hand and left-hand limits of function ψ(s) at time s, respectively. In particular, let 𝑃𝐡 β‰œ

𝑃𝐡 [βˆ’πœ, 0], ℝ :

β„‹ = {β„Ž(𝑠): ℝ β†’ ℝ ∣

β„Ž(𝑠)𝑖𝑠 π‘–π‘›π‘‘π‘’π‘”π‘Ÿπ‘Žπ‘™ π‘Žπ‘›π‘‘ π‘ π‘Žπ‘‘π‘–π‘ π‘“π‘–π‘’π‘  sup ∫ β„Ž(𝑠)𝑑𝑠 =

𝐻 < ∞, π‘Žπ‘›π‘‘ lim β†’βˆž ∫ β„Ž(𝑠)𝑑𝑠 =

∞, π‘€β„Žπ‘’π‘Ÿπ‘’ 𝐻 𝑖𝑠 π‘Ž π‘π‘œπ‘ π‘–π‘‘π‘–π‘£π‘’ π‘π‘œπ‘›π‘ π‘‘π‘Žπ‘›π‘‘}.

For πœ‘ ∈ 𝐡[𝕁, ℝ ] π‘œπ‘Ÿ πœ‘ ∈ 𝑃𝐡[𝕁, ℝ ], we define[πœ‘(𝑑)] = ([πœ‘ (𝑑)] , … , [πœ‘ (𝑑)] ) , [πœ‘ (𝑑)] = sup {πœ‘ (𝑑 + 𝑠)}, 𝑖 ∈ 𝒩, And 𝐷 πœ‘(𝑑) denotes the upper right-hand derivative of πœ‘(𝑑) at time t.

Let (Ξ©, β„±, {β„± } , 𝑃) be a complete probability space with a filtration {β„± } satisfying the usual conditions ( i.e., it is right continuous and β„± contains all p-null sets ). Let 𝑃𝐡ℱ [βˆ’πœ, 0], ℝ (𝑃𝐡ℱ [βˆ’πœ, 0], ℝ ) denote the family of all bounded β„± (β„± )-measurable, 𝑃𝐡 [βˆ’πœ, 0], ℝ -valued random variable πœ™, satisfying β€–πœ™β€– = sup 𝔼|πœ™(πœƒ)| < ∞, where 𝔼 denotes the expectation of stochastic process. Let β„’ denote the well-known β„’-operator given by the Ito formula.

In this paper, we consider the following Ito impetuous stochastic delay systems:

⎩βŽͺ⎨

βŽͺ⎧ 𝑑π‘₯(𝑑) = 𝐴(𝑑)π‘₯(𝑑) + 𝑓 𝑑, π‘₯ 𝑑 βˆ’ 𝜏(𝑑) 𝑑𝑑 +

𝜎 𝑑, π‘₯(𝑑), π‘₯ 𝑑 βˆ’ 𝜏(𝑑) 𝑑𝑀(𝑑), 𝑑 β‰  𝑑 , 𝑑 β‰₯ 𝑑 ,

βˆ†π‘₯ = π‘₯(𝑑 ) βˆ’ π‘₯(𝑑 ) = 𝐼 π‘₯(𝑑 ),

π‘₯(𝑑 + 𝑠) = πœ™(𝑠), 𝑠 ∈ [βˆ’πœ, 0],

 

(1)

Where the initial function

πœ™(𝑠) = πœ™ (𝑠), … , πœ™ (𝑠) ∈ 𝑃𝐡ℱ [βˆ’πœ, 0], ℝ .

𝐴(𝑑) = β„Ž(𝑑)𝐴, β„Ž(𝑑) ∈ β„‹, 𝐴 ∈ ℝ Γ— . 𝐼 ∈ ℝ Γ— , 0 β‰€πœ(𝑑) ≀ 𝜏, 𝜏 𝑖𝑠 π‘Ž π‘π‘œπ‘›π‘ π‘‘π‘Žπ‘›π‘‘, and fixed impetuous moment 𝑑 (π‘˜ ∈ β„•) satisfy 𝑑 < 𝑑 < β‹― and lim β†’βˆž 𝑑 = ∞. 𝑓: ℝ Γ— ℝ β†’ ℝ π‘Žπ‘›π‘‘ 𝜎: ℝ Γ— ℝ ×ℝ β†’ ℝ Γ— are piecewise continuous vector-valued functions with 𝑓(𝑑, 0) = 𝜎(𝑑, 0,0) ≑ 0, 𝑑 ∈ ℝ , and ensuring the existence and uniqueness of (1). One may refer to[9,10] for the results on the existence and uniqueness of solutions of impetuous stochastic system.

The solution π‘₯(𝑑) = π‘₯ (𝑑), … , π‘₯ (𝑑) is a PB –valued stochastic process.

𝑀(𝑑) = 𝑀 (𝑑), … , 𝑀 (𝑑) is an m-dimensional Brownian motion defined (Ξ©, β„±, {β„± } , 𝑃).

Definition 2.1

The trivial solution of (1) is said to be globally mean square asymptotically stable if for any given initial condition πœ™ ∈ 𝑃𝐡ℱ [βˆ’πœ, 0], ℝ such that

limβ†’βˆž

𝔼|π‘₯(𝑑, 𝑑 , πœ™)| = 0.

Definition 2.2

The trivial solution of (1) is said to be globally mean square exponentially stable if there exist constants πœ† > 0 and π‘˜ > 1 such that for any solution x(t) with the initial condition πœ™ ∈ 𝑃𝐡ℱ [βˆ’πœ, 0], ℝ ,

𝔼|π‘₯(𝑑)| ≀ π‘˜β€–πœ™β€– 𝑒 ( ), 𝑑 β‰₯ 𝑑 .

3. Main results

In this section, we will first projecting an impetuous differential inequality with delays and then investigate the mean square stability of (1) by employing the obtained impetuous differential inequality, and stochastic analysis technique. It is shown that an unstable stochastic delays system can be successfully stabilized by impetuous.

Theorem 3.1

Let π‘ž β‰₯ 0, and 𝑋(𝑑), π‘Œ(𝑑) ∈ 𝑃𝐡[[𝑑 , ∞), ℝ] be a solution of the following impetuous delay differential inequality with the initial condition 𝑋(𝑑), π‘Œ(𝑑) βˆˆπ‘ƒπ΅, βˆ’πœ ≀ 𝑠 ≀ 𝑑 ,

Page 3: Time Delay and Mean Square Stochastic Differential Equations in Impetuous Stabilization

International Journal of Trend in Scientific Research and Development (IJTSRD) ISSN: 2456-6470

@ IJTSRD | Available Online @ www.ijtsrd.com | Volume – 2 | Issue – 3 | Mar-Apr 2018 Page: 629

𝐷 𝑋(𝑑) ≀ β„Ž(𝑑)[βˆ’π‘ƒπ‘‹(𝑑) + π‘ž[𝑋(𝑑)] ], 𝑑 β‰  𝑑 , 𝑑 β‰₯ 𝑑

𝑋(𝑑 ) ≀ 𝛼 𝑋(𝑑̅ ), 0 < 𝛼 < 1, π‘˜ ∈ β„•,

𝑋(𝑑 + 𝑠) = πœ™(𝑠) ∈ 𝑃𝐡 [βˆ’πœ, 0], ℝ βˆ’ 𝜏 ≀ 𝑠 ≀ 0

 

+

𝐷 π‘Œ(𝑑) ≀ β„Ž(𝑑)[βˆ’π‘ƒπ‘Œ(𝑑) + π‘ž[π‘Œ(𝑑)] ], 𝑑 β‰  𝑑 , 𝑑 β‰₯ 𝑑

π‘Œ(𝑑 ) ≀ 𝛼 π‘Œ(𝑑̅ ), 0 < 𝛼 < 1, 𝑛 ∈ β„•,

π‘Œ(𝑑 + 𝑠) = πœ™(𝑠) ∈ 𝑃𝐡 [βˆ’πœ, 0], ℝ βˆ’ 𝜏 ≀ 𝑠 ≀ 0

 

(2)

Where β„Ž(𝑑) ∈ β„‹. Assume that the following condition is satisfied

βˆ’π‘ + ∫ β„Ž(𝑠)𝑑𝑠 +

βˆ’π‘ + ∫ β„Ž(𝑠)𝑑𝑠 < βˆ’πΌπ‘›π›Ό βˆ’ 𝐼𝑛𝛼 ,

π‘˜ ∈ β„•. (3)

Then there exist a constant 𝑀 β‰₯ 1, 𝐺 β‰₯ 1 and a small enough number πœ† > 0, πœ‡ > 0 such that

𝑋(𝑑) + π‘Œ(𝑑) ≀

β€–πœ™β€–π‘€π‘’βˆ« β„Ž( )

+ β€–πœ™β€–πΊπ‘’βˆ« β„Ž( )

, 𝑑 β‰₯ 𝑑 (4)

Where β€–πœ™β€– = sup |πœ™(𝑠)|, and the constants πœ† > 0, πœ‡ > 0 satisfies the following inequality

2πœ† βˆ’ 𝑝 + ∫ β„Ž(𝑠)𝑑𝑠 + 2πœ‡ βˆ’ 𝑝 +

∫ β„Ž(𝑠)𝑑𝑠 < βˆ’πΌπ‘›π›Ό βˆ’ 𝐼𝑛𝛼 , π‘˜ ∈

β„•, 𝑛 ∈ β„•. (5)

Proof

We shall show that

𝑋(𝑑) + π‘Œ(𝑑) ≀

β€–πœ™β€–π‘€π‘’βˆ« β„Ž( )

+ β€–πœ™β€–πΊπ‘’βˆ« β„Ž( )

, 𝑑 ∈[𝑑 , 𝑑 ), π‘˜ ∈ β„• & 𝑑 ∈ [𝑑 , 𝑑 ), 𝑛 βˆˆβ„•. (6)

By using the continuity, from (3) we know that there must there must exist a positive constants πœ† π‘Žπ‘›π‘‘ πœ‡ such that for all (5) holds.

Let 𝛾 = 𝑠𝑒𝑝 βˆˆβ„•{ } β‰₯ 1 and 𝛿 =

𝑠𝑒𝑝 βˆˆβ„•{ } β‰₯ 1 in (5), then we can select constant

πœ‚ > 0, 𝜌 > 0 such that for all π‘˜ ∈ β„•, 𝑛 ∈ β„•.

βˆ’2𝑝 + π›Ύπ‘žπ‘’ + π›Ώπ‘žπ‘’ < βˆ’πΌπ‘›π›Ό βˆ’ 𝐼𝑛𝛼 , π‘˜ βˆˆβ„•, 𝑛 ∈ β„•. (7)

And

(πœ‚ + πœ†) ∫ β„Ž(𝑠)𝑑𝑠 + (𝜌 + πœ‡) ∫ β„Ž(𝑠)𝑑𝑠 <

βˆ’πΌπ‘›π›Ό βˆ’ 𝐼𝑛𝛼 ≀ 𝐼𝑛𝛾 + 𝐼𝑛𝛿 (8)

From (8) we can choose 𝑀 β‰₯ 1, 𝐺 β‰₯ 1 such that

1 < 𝑒( ) ∫ β„Ž( )

+ 𝑒( ) ∫ β„Ž( )

≀ 𝑀 + 𝐺 ≀

𝛾𝑒( ) ∫ β„Ž( )

𝑒( ) ∫ β„Ž( )

+

𝛿𝑒( ) ∫ β„Ž( )

𝑒( ) ∫ β„Ž( )

. (9)

It then follows that

β€–πœ™β€– < β€–πœ™β€–π‘’βˆ« β„Ž( )

+ β€–πœ™β€–π‘’βˆ« β„Ž( )

≀ β€–πœ™β€–π‘€π‘’βˆ« β„Ž( )

+ β€–πœ™β€–πΊπ‘’βˆ« β„Ž( )

(10)

We first prove that

𝑋(𝑑) + π‘Œ(𝑑) ≀

β€–πœ™β€–π‘€π‘’βˆ« β„Ž( )

+ β€–πœ™β€–πΊπ‘’βˆ« β„Ž( )

, 𝑑 ∈[𝑑 , 𝑑 ). (11)

To do this, we only to prove that

𝑋(𝑑) + π‘Œ(𝑑)

≀ β€–πœ™β€–π‘€π‘’βˆ« β„Ž( )

+ β€–πœ™β€–πΊπ‘’βˆ« β„Ž( )

(12)

If (12) is not true, by (10), then there exists some 𝑑̅ ∈ (𝑑 , 𝑑 ) such that

𝑋(𝑑)Μ… + π‘Œ(𝑑)Μ… > β€–πœ™β€–π‘€π‘’βˆ« β„Ž( )

+ β€–πœ™β€–πΊπ‘’βˆ« β„Ž( )

β‰₯ β€–πœ™β€–π‘’βˆ« β„Ž( )

+ β€–πœ™β€–π‘’βˆ« β„Ž( )

> β€–πœ™β€– β‰₯ 𝑒(𝑑 + 𝑠), 𝑠 ∈ [βˆ’πœ, 0]

(13)

Which implies that there exists some π‘‘βˆ— ∈ (𝑑 , 𝑑̅) such that

𝑋(π‘‘βˆ—) + π‘Œ(π‘‘βˆ—) =

β€–πœ™β€–π‘€π‘’βˆ« β„Ž( )

+ β€–πœ™β€–πΊπ‘’βˆ« β„Ž( )

,π‘Žπ‘›π‘‘ 𝑋(𝑑) + π‘Œ(𝑑) ≀ 𝑋(π‘‘βˆ—) + π‘Œ(π‘‘βˆ—), 𝑑 ∈ [𝑑 βˆ’ 𝜏, π‘‘βˆ—] (14)

Page 4: Time Delay and Mean Square Stochastic Differential Equations in Impetuous Stabilization

International Journal of Trend in Scientific Research and Development (IJTSRD) ISSN: 2456-6470

@ IJTSRD | Available Online @ www.ijtsrd.com | Volume – 2 | Issue – 3 | Mar-Apr 2018 Page: 630

And there exists π‘‘βˆ—βˆ— ∈ [𝑑 , π‘‘βˆ—) such that

𝑋(π‘‘βˆ—βˆ—) + π‘Œ(π‘‘βˆ—βˆ—) = β€–πœ™β€–, π‘Žπ‘›π‘‘ 𝑋(π‘‘βˆ—βˆ—) + π‘Œ(π‘‘βˆ—βˆ—) ≀𝑋(𝑑) + π‘Œ(𝑑) ≀ 𝑋(π‘‘βˆ—) + π‘Œ(π‘‘βˆ—), 𝑑 ∈ [π‘‘βˆ—βˆ—, π‘‘βˆ—]. (15)

Hence, we get for any 𝑠 ∈ [βˆ’πœ, 0],

𝑋(𝑑 + 𝑠) + π‘Œ(𝑑 + 𝑠)

≀ β€–πœ™β€–π‘€π‘’βˆ« β„Ž( )

+ β€–πœ™β€–πΊπ‘’βˆ« β„Ž( )

≀ β€–πœ™β€–π›Ύπ‘’( ) ∫ β„Ž( )

𝑒( ) ∫ β„Ž( )

+ β€–πœ™β€–π›Ώπ‘’( ) ∫ β„Ž( )

𝑒( ) ∫ β„Ž( )

= 𝛾𝑒 𝑋(π‘‘βˆ—βˆ—) + 𝛿𝑒 π‘Œ ≀ 𝛾𝑒 𝑋(𝑑) + 𝛿𝑒 π‘Œ(𝑑),𝑑 ∈ [π‘‘βˆ—βˆ—, π‘‘βˆ—]. (16)

Thus, by (7) and (16), we have

𝐷 𝑋(𝑑) ≀ β„Ž(𝑑)[βˆ’π‘π‘‹(𝑑) + π‘ž[𝑋(𝑑)] ] ≀ β„Ž(𝑑) βˆ’π‘ +

π›Ύπ‘žπ‘’ ]𝑋(𝑑) ≀ β„Ž(𝑑)(πœ‚ βˆ’ πœ†)𝑋(𝑑), 𝑑 ∈ [π‘‘βˆ—βˆ—, π‘‘βˆ—] + 𝐷 π‘Œ(𝑑) ≀ β„Ž(𝑑)[βˆ’π‘π‘Œ(𝑑) + π‘ž[π‘Œ(𝑑)] ]

≀ β„Ž(𝑑)[βˆ’π‘ + π›Ώπ‘žπ‘’ ]π‘Œ(𝑑) ≀ β„Ž(𝑑)(𝜌 βˆ’ πœ‡)π‘Œ(𝑑), 𝑑 ∈[π‘‘βˆ—βˆ—, π‘‘βˆ—] (17)

It follows from (10),(14) and (15) that

𝑋(π‘‘βˆ—) + π‘Œ(π‘‘βˆ—) ≀ 𝑋(π‘‘βˆ—βˆ—)𝑒( ) ∫ β„Ž( )βˆ—

βˆ—βˆ— +

π‘Œ(π‘‘βˆ—βˆ—)𝑒( ) ∫ β„Ž( )βˆ—

βˆ—βˆ— < β€–πœ™β€–π‘’βˆ« β„Ž( )

+

β€–πœ™β€–π‘’βˆ« β„Ž( )

≀ β€–πœ™β€–π‘€π‘’βˆ« β„Ž( )

+

β€–πœ™β€–πΊπ‘’βˆ« β„Ž( )

= 𝑋(π‘‘βˆ—) + π‘Œ(π‘‘βˆ—)

(18)

Which is contradiction. Hence (12) holds and then (6) is true for π‘˜ = 1. Now we assume that (6) holds for π‘˜ = 1,2, … , π‘š(π‘š ∈ β„•, π‘š β‰₯ 1),

𝑋(𝑑) + π‘Œ(𝑑) ≀

β€–πœ™β€–π‘€π‘’βˆ« β„Ž( )

+ β€–πœ™β€–πΊπ‘’βˆ« β„Ž( )

, 𝑑 ∈[𝑑 , 𝑑 ),

π‘˜ = 1,2, … , π‘š.

(19)

Next, To find equation (6) holds for π‘˜ = π‘š + 1, (𝑑) + π‘Œ(𝑑) ≀

β€–πœ™β€–π‘€π‘’βˆ« β„Ž( )

+ β€–πœ™β€–πΊπ‘’βˆ« β„Ž( )

, 𝑑 ∈[𝑑 , 𝑑 ).

(20)

For the reasons of contradiction, suppose (20) is not true. Then we define

𝑑̅ =inf{𝑑 ∈ [𝑑 , 𝑑 )|𝑋(𝑑) + π‘Œ(𝑑) >

β€–πœ™β€–π‘€π‘’βˆ« β„Ž( )

+ β€–πœ™β€–πΊπ‘’βˆ« β„Ž( )

}.

(21)

By (8) and (19), we have

𝑋(𝑑 ) + π‘Œ(𝑑 )

≀ 𝛼 β€–πœ™β€–π‘€π‘’βˆ« β„Ž( )

+ 𝛼 β€–πœ™β€–πΊπ‘’βˆ« β„Ž( )

< 𝛼 π‘’βˆ« β„Ž( )

β€–πœ™β€–π‘€π‘’βˆ« β„Ž( )

+ 𝛼 π‘’βˆ« β„Ž( )

β€–πœ™β€–πΊπ‘’βˆ« β„Ž( )

< β€–πœ™β€–π‘€π‘’βˆ« β„Ž( )

+ β€–πœ™β€–πΊπ‘’βˆ« β„Ž( )

, (22)

And so 𝑑̅ β‰  𝑑 . By utilizing the continuity of 𝑋(𝑑) + π‘Œ(𝑑) in the interval [𝑑 , 𝑑 ), we get

𝑋(𝑑)Μ… + π‘Œ(𝑑)Μ… =

β€–πœ™β€–π‘€π‘’βˆ« β„Ž( )

+ β€–πœ™β€–πΊπ‘’βˆ« β„Ž( )

, π‘Žπ‘›π‘‘ 𝑋(𝑑) +π‘Œ(𝑑) ≀ 𝑋(𝑑)Μ… + π‘Œ(𝑑)Μ…, 𝑑 ∈ [𝑑 , 𝑑̅]. (23)

From (22), we know that there exist some π‘‘βˆ— ∈ (𝑑 , 𝑑̅) such that

𝑋(π‘‘βˆ—) + π‘Œ(π‘‘βˆ—) =

𝛼 π‘’βˆ« β„Ž( )

β€–πœ™β€–π‘€π‘’βˆ« β„Ž( )

+

𝛼 π‘’βˆ« β„Ž( )

β€–πœ™β€–πΊπ‘’βˆ« β„Ž( )

,

π‘Žπ‘›π‘‘ 𝑋(π‘‘βˆ—) + π‘Œ(π‘‘βˆ—) ≀ 𝑋(𝑑) + π‘Œ(𝑑) ≀𝑋(𝑑)Μ… + π‘Œ(𝑑)Μ…, 𝑑 ∈ [𝑑 , 𝑑̅]. (24)

On the other hand, for any 𝑑 ∈ [π‘‘βˆ—, 𝑑]Μ… , 𝑠 ∈[βˆ’πœ, 0], either 𝑑 + 𝑠 ∈ [𝑑 βˆ’ 𝜏, 𝑑 )π‘œπ‘Ÿ 𝑑 + 𝑠 ∈ [𝑑 , 𝑑̅]. Two cases will be discussed as follows. If 𝑑 + 𝑠 ∈[𝑑 βˆ’ 𝜏, 𝑑 ), from (19),we obtain 𝑋(𝑑 + 𝑠) +

π‘Œ(𝑑 + 𝑠) ≀ β€–πœ™β€–π‘€π‘’βˆ« β„Ž( )

𝑒 ∫ β„Ž( ) +

β€–πœ™β€–πΊπ‘’βˆ« β„Ž( )

𝑒 ∫ β„Ž( ) ≀

β€–πœ™β€–π‘€π‘’βˆ« β„Ž( )

𝑒 +

β€–πœ™β€–πΊπ‘’βˆ« β„Ž( )

𝑒

≀ β€–πœ™β€–π‘’ π‘’βˆ« β„Ž( )

π‘€π‘’βˆ« β„Ž( )

+

Page 5: Time Delay and Mean Square Stochastic Differential Equations in Impetuous Stabilization

International Journal of Trend in Scientific Research and Development (IJTSRD) ISSN: 2456-6470

@ IJTSRD | Available Online @ www.ijtsrd.com | Volume – 2 | Issue – 3 | Mar-Apr 2018 Page: 631

β€–πœ™β€–π‘’ π‘’βˆ« β„Ž( )

πΊπ‘’βˆ« β„Ž( )

(25)

if 𝑑 + 𝑠 ∈ [𝑑 , 𝑑̅], form (23), then

𝑋(𝑑 + 𝑠) + π‘Œ(𝑑 + 𝑠) = β€–πœ™β€–π‘€π‘’βˆ« β„Ž( )

+

β€–πœ™β€–πΊπ‘’βˆ« β„Ž( )

≀

β€–πœ™β€–π‘’ π‘’βˆ« β„Ž( )

π‘€π‘’βˆ« β„Ž( )

+

β€–πœ™β€–π‘’ π‘’βˆ« β„Ž( )

πΊπ‘’βˆ« β„Ž( )

(26) (26)

In any case, from (24)-(26), we all have for any 𝑠 ∈ [βˆ’πœ, 0],

𝑐[𝑋(𝑑 + 𝑠) + π‘Œ(𝑑 + 𝑠)] ≀ 𝑋(π‘‘βˆ—) + π‘Œ(π‘‘βˆ—) ≀

𝛾𝑒 𝑋(𝑑) + 𝛿𝑒 π‘Œ(𝑑), 𝑑 ∈ [π‘‘βˆ—, 𝑑̅] , (27)

Finally, by (7) and (27), we all have

𝐷 [𝑋(𝑑) + π‘Œ(𝑑)] ≀ β„Ž(𝑑)[(πœ‚ βˆ’ πœ†)𝑋(𝑑) +πœŒβˆ’πœ‡π‘Œπ‘‘. (28)

It follows from (8), (23) and (24) that

𝑋(𝑑)Μ… + π‘Œ(𝑑̅)

≀ 𝑋(π‘‘βˆ—)𝑒( ) ∫ β„Ž( )βˆ—

+ π‘Œ(π‘‘βˆ—)𝑒( ) ∫ β„Ž( )βˆ—

< 𝑒( ) ∫ β„Ž( )

π‘’βˆ« β„Ž( )

β€–πœ™β€–π‘€π‘’βˆ« β„Ž( )

+ 𝑒( ) ∫ β„Ž( )

π‘’βˆ« β„Ž( )

β€–πœ™β€–πΊ

< β€–πœ™β€–π‘€π‘’βˆ« β„Ž( )

+ β€–πœ™β€–πΊπ‘’βˆ« β„Ž( )

= 𝑋(𝑑)Μ… + π‘Œ(𝑑̅) (29)

Which is a contradiction. This implies that the assumption is not true, and hence (6) holds for π‘˜ = π‘š + 1. Therefore, by some simple mathematical induction, we can obtain that (6) holds for any π‘˜ ∈ β„•. This completes the proof of theorem.

References

1) Z.G. Yang, D.Y.Xu, L.Xiang, Exponential p-stability of impulsive stochastic differential equations with delays, Phys. Lett. A 359 (2006) 129-137.

2) L.G.Xu, D.Y.Xu, p-attracting and p-invariant sets for a class of impulsive stochastic functional differential equations, comput. Math. Appl. 57 (2009) 54-61.

3) L.G.Xu, D.Y.Xu, Exponential p-stability of impulsive stochastic neural networks with mixed delays, Chaos Solitons Fractals 41(2009) 263-272.

4) L.G.Xu, Exponential p-stability of singularly perturbed impulsive stochastic delay differential systems, Int. J. Control Autom. 9 (2011) 966-972.

5) L.G.Xu, D.H.He, Mean square exponential stability analysis of impulsive stochastic switched systems with mixed delays, comput. Math. Appl. 62 (2011) 109-117.

6) J.Liu, X.Z.Liu, W.C.Xie, Impulsive stabilization of stochastic functional differential equations, Appl. Math. Lett. 24 (2011) 264-269.

7) J.Zhou, Q.J.Wu, L.Xiang, et al., Impulsive synchronization seeking in general complex delayed dynamical networks, Nonlinear Anal. Hybrid Sys. 5 (2011) 513-524.

8) Z.G. Yang, Z.C. Yang, Dissipativity in mean square of non- autonomous impulsive stochastic neural networks with delays, Lecture Notes in Comput. Sci. 6063 (2010) 735-744.

9) B.Liu, X.Z.Liu, X.X.Liao, Existence and uniqueness and stability of solutions for stochastic impulsive systems, J.Syst. Sci. Complex. 20 (2007) 149-158.

10) M.S.Alwan, X.Z.Liu, W.Xie, Existence, continuation and uniqueness problems of stochastic impulsive systems with time delay, J.Franklin Inst. 347 (2010) 1317-1333.

11) X.Z.Liu, A.R.Willms, impulsive controllability of linear dynamical systems with applications to maneuvers of spacecraft, Math. Probl. Eng. 2 (1996) 277-299.

12) D.Bainov, P.S.Simeonov, Systems with impulse Effect: Stability, Theory and Applications, Ellis Horwood Limited, Chichester, 1989.

13) X.Z.Liu, K.Rohlf, Impulsive control of a Lotka-Volterra system, IMAJ. Math. Control Inform. 15 (1998) 269-284.

14) V.Lakshmikantham, D.D.Bainov, P.S.Simeonov, Theory of Impulsive Differential Equations, World Scientific, Singapore, 1989.

15) A. Khadra, X.Z.Liu, X.M.Shen, Application of impulsive synchronization to communication security, IEEE Trans. Circuits Syst. I 50 (2003) 341-351.

16) J.T.Sun, Impulsive control of a new chaotic system, Math. Comput. Simul. 64 (2004) 669-677.