Volume 2012, Issue 1 804509
Research Article
Open Access

Asymptotic Stability of Differential Equations with Infinite Delay

D. Piriadarshani

Corresponding Author

D. Piriadarshani

Department of Mathematics, Hindustan Institute of Technology and Science, Rajiv Gandhi Salai, Kelambakkam, Chennai 603 103, India hindustanuniv.ac.in

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T. Sengadir

T. Sengadir

Department of Mathematics, Central University of Tamil Nadu, Thiruvarur 610 004, India cutn.ac.in

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First published: 31 May 2012
Academic Editor: Mehmet Sezer

Abstract

A theorem on asymptotic stability is obtained for a differential equation with an infinite delay in a function space which is suitable for the numerical computation of the solution to the infinite delay equation.

1. Introduction and Preliminaries

In this paper, we study the asymptotic stability of the solutions to the infinite delay differential equation given below:
()
under the following assumptions.
  • (i)

    There exists p > 0 with |bi | ≤ pγi for all i.

  • (ii)

    τiiτ1 for all i  .

The asymptotic stability of a linear infinite delay equation is studied in [15] in the context of abstract phase spaces which includes the space:
()
The asymptotic constancy neutral equations are studied in [6]. Linear time-invariant systems with constant point delays are studied in [7] and in [8]; a Razumikhin approach is used to study exponential stability of delay equations. Asymptotic stability and stabilization of linear delay-differential equations are studied in [9].
In this paper, the phase space Cσ(−, 0] for the initial function is chosen as follows. Let mi = iτ1 > 0 and βi = pγi. The space Cσ(−, 0] is defined as
()
Here C(−, 0] is the set of continuous complex valued functions defined on (−, 0].

The motivation to consider the above type of phase space is that for numerical computation of solutions it is enough to know the values of the initial data over a finite domain at every stage of computation. See [10, 11].

The following definitions and results are well known, see for example [5] or [12].

Definition 1.1. The Kuratowski measure of noncompactness α(V) of the subset V of a Banach space X is defined by

()
For a bounded linear operator L : XY, |L|α is defined as
()

Proposition 1.2. Let X, Y, Z be Banach spaces and M : XY, L : YZ be bounded linear operators. Then, |ML|α≤|M|α | L|α. Further, if M : XY is compact, then |M|α = 0.

Theorem 1.3. Let X be a Banach space and let A : D(A) → X be the infinitesimal generator of a semigroup of operators St : XX. Then, the growth bound of the semigroup ω0 defined as

()
is given by
()
where s(A) = sup {(λ) : λ ∈ spec (A)} and
()

In Theorem 1.3, spec(A) is the compliment of the resolvent set ρ(A) which is the set of all λC such that the operator λIA is one-one and onto and (λIA) −1 is a bounded linear map.

For a real number r, ⌊r⌋ = max {nZ : nr} and ⌈r⌉ = min   {nZ : nr}. We will make use of the observation ⌈r⌉ ≤ ⌊r⌋ ≤ r + 1 for r.

2. Asymptotic Stability of a PDE

Consider the following simple initial boundary value problem for a PDE:
()
where u0Cσ,0(−, 0] = {uCσ(−, 0] : u(0) = 0}.
Its mild solution is given by the semigroup Tt : Cσ,0(−, 0] → Cσ,0(−, 0] defined as
()

Proposition 2.1. Let mi = iτ1 and βi = pγi. The infinitesimal generator of the semigroup defined by (2.2) is given by B : D(B) → Cσ,0(−, 0], Bϕ = ϕ, where

()
Further, ρ(B) = {λ : (λ)>−ln  γ/τ1}.

Besides, if (λ)>−ln  γ/τ1, then eλCσ(−, 0] and for every fCσ(−, 0], h defined as and eλ defined as eλ(θ) = eλθ are elements of Cσ(−, 0].

Finally, for the semigroup Tt defined in (2.2), ω0 = −ln  γ/τ1.

Proof. Since θ ∈ [−iτ1, 0]⇒t + θ ∈ [−iτ1, t],

()
and hence ∥Ttσ ≤ 1, Tt+s = TtTs is obvious, then
()
can be proved using Proposition 1.9 of [10]. The proof that B is the infinitesimal generator of Tt is also easy.

Note that λ = 0 trivially satisfies (λ)>−ln  γ/τ1. Let 0 ≠ λρ(B). Define ϕ, as ϕ(θ) = θ. Since , ϕCσ,0(−, 0] and hence there is a unique ψD(B), such that λψψ = ϕ. Indeed, ψ = (λI0B) −1ϕ. Here, I0 is the identity on Cσ,0(−, 0]. Let us note that ψ(0) = 0. Now, we find that ψ1, defined as ψ1(θ) = θ/λ + (1/λ2)(1 − eλθ) is the unique continuously differentiable function such that and ψ1(0) = 0. From this we infer that ψ1 = (λI0B) −1ϕ and hence ψ1Cσ,0(−, 0]. Now, since ϕCσ,0(−, 0], we obtain (1 − eλ) ∈ Cσ,0(−, 0]⊆Cσ(−, 0]. Since the constant function 1 is an element of Cσ(−, 0], eλCσ(−, 0]. Noting that −ln  γ/τ1 = inf  {(λ) : eλCσ(−, 0]}, we obtain (λ)>−ln  γ/τ1.

Let tτ1. It is clear that for all i ≤ ⌊t/τ1⌋, and θ ∈ [−iτ1, 0], Ttϕ(θ) = 0. For i > ⌊t/τ1⌋, and θ ∈ [−iτ1, 0], we have t + θtiτ1 ≥ −(i − ⌊t/τ1⌋)τ1. Thus,
()
Hence
()

Hence, the operator norm .

To prove the equality, we construct a function ηCσ,0(−, 0] such that and the result follows.

Let δ = (⌊t/τ1  ⌋ + 1)τ1t = τ1(⌊t/τ1  ⌋ + 1 − t/τ1). We have, δ < τ1. Define,
()
It is clear that, Now,
()
Thus .

Hence, .

Now, ω0 = lim t(1/t)ln (∥Ttσ) = −ln (γ)/τ1.

Let (λ)>−ln  γ/τ1. Since
()
we have λρ(B).

Let fCσ(−, 0]. Define g(θ) = f(θ) − f(0). Then gCσ,0(−, 0].

Let ψ = (λI0B) −1g. We have, ψ(0) = 0.

Define . Now ψ1(0) = 0 and .

By the uniqueness of the solution to the initial value problem of the ODE:
()
it is now obvious that ψ1 = ψ and hence ψ1Cσ,0(−, 0].
Now,
()
Since 1 − eλCσ,0(−, 0], hCσ,0(−, 0] ⊂ Cσ(−, 0], where h is defined as .

3. Stability of the Infinite Delay Equation

The proof of the next theorem assuring the existence of a unique solution to (1.1) is similar to the proof of Theorem 2.2 of [10].

Theorem 3.1. Let a and the sequences bi and βi be as in Section 1. Assume that τiiτ1. Then there exists a unique solution x : to (1.1) such that its restriction to [0, ), denoted by y, is in C1[0, ). Further, for any t ∈ [0, ), there is a constant c(t) > 0 such that

()

In addition, the family of operators {St : t ≥ 0} defined as
()
forms a semigroup. Also, the infinitesimal generator of St is given by A : D(A) → Cσ(−, 0], where
()
Further, D(A) is dense and A is a closed operator.

Theorem 3.2. For the semigroup St defined by (3.2)

()

Further, assume that . Then for the generator of the semigroup St defined by (3.3) and
()

Besides, suppose that for any λC with , we have (λ)<−μ1 for some μ1 > 0. Then, the semigroup St is asymptotically stable.

Proof. Let Tt be as in Proposition 2.1. Fix t > 0. Define Vt : Cσ(−, 0] → Cσ(−, 0] as

()
Define Kt : C[0, t] → Cσ(−, 0] as
()

It is easy to see that
()
Thus, Kt is a bounded linear map.
Define K1 : Cσ(−, 0] → Cσ(−, 0] as [K1ϕ](θ) = ϕ(0) for all θ ∈ (−, 0]. It is clear that K1 is compact. Define Bt : Cσ(−, 0] → C[0, t] as Btϕ = z, where z is the restriction of y to [0, t]. From (3.1), Bt is a bounded linear map. Let St be as in (3.3). Then,
()
Now, if I is the identity on Cσ(−, 0] and J : Cσ,0(−, 0] → Cσ(−, 0] is the inclusion map, then Vt = JTt(IK1), and, finally,
()
Next, we show that Bt is, in fact, a compact map. Let x be the solution to (1.1) as in Theorem 3.1:
()
Thus,
()
Consider n such that t ∈ [nτ1, (n + 1)τ1]. From (3.1) and (3.11), we obtain existence of c1(t) ≥ 0 such that
()

Hence by Arzela-Ascoli theorem, Bt is a compact operator.

It is easy to show that |J|α ≤ ∥Jσ = 1. By the compactness of K1 and Bt, |IK1|α = 1 and |KtBt|α = |K1|α = 0. Thus, from the relation
()
and Propositions 1.2 and 2.1 of this paper, we obtain
()
So,
()

Let 0 ≠ λρ(A).

There is a unique ψD(A) such that
()
It is clear that there is cC such that ψ(θ) = (c − 1/λ)eλθ − 1/λ. Now, we claim that c ≠ 1/λ. If c = 1/λ, then ψ(θ) = −1/λ for all θ ∈ (−, 0]. Since ψD(A), we must have . But this would imply that which is a contradiction, to the hypothesis that . Now, since c − 1/λ ≠ 0, it is obvious that eλCσ(−, 0]. But this implies that (λ)>−ln  (γ)/τ1. If 0 ∈ ρ(A), the condition (λ)>−ln  (γ)/τ1 is obvious. Thus,
()
We now infer that {λ : (λ)≤−ln (γ)/τ1}⊆spec(A). Next, if , and (λ)>−ln  (γ)/τ1, then eλCσ(−, 0] and hence eλD(A) with λeλ = Aeλ. Thus, λ ∈ spec(A). So,
()

Let us assume that (λ)>−ln  (γ)/τ1 and .

Then, by Proposition 2.1, we have eλCσ(−, 0] and the function h defined as is in Cσ(−, 0].

Defining Λ : Cσ(−, 0] → C as and taking c = (Λ(h) − f(0))/(Λ(eλ) − λ), we find that ϕ defined as is (λIA) −1(f). Thus,
()
From (3.18), (3.19), and (3.20), we finally conclude that
()
or
()
Since ω0 = max {s(A), ωess} ≤ max {−μ1, −ln (γ)/τ1}, the result follows.

Remark 3.3. Consider the PDE:

()
Let B be as in Proposition 2.1 and A be as in Theorem 3.1. For ϕD(B), u(t, θ) = TtϕCσ,0(−, 0] is the solution to the above PDE. For ϕD(A), u(t, θ) = StϕCσ(−, 0] is the solution to the above PDE. For the first solution u(t + θ) = 0, t + θ ≥ 0 and for the second solution u(t + θ) = x(t + θ), t + θ ≥ 0. Here x is the solution to the delay equation.

Acknowledgment

D. Piriadarshani would like to thank Professor B. Praba, Department of Mathematics, SSN College of Engineering, Kalavakkam, Tamil Nadu, India, for the support and advice received from her as a Cosupervisor.

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