Controllability of Impulsive Semilinear Stochastic Heat Equation with Delay
Abstract
LaSalle wrote the following: “it is never possible to start the system exactly in its equilibrium state, and the system is always subject to outside forces not taken into account by the differential equations. The system is disturbed and is displaced slightly from its equilibrium state. What happens? Does it remain near the equilibrium state? This is stability. Does it remain near the equilibrium state and in addition tend to return to the equilibrium? This is asymptotic stability.” Continuing with what LaSalle said, we conjecture that real-life systems are always under the influence of impulses, delays, memory, nonlocal conditions, and noises, which are intrinsic phenomena no taken into account by the mathematical model that is representing by a differential equation. For many control systems in real life, delays, impulses, and noises are natural properties that do not change their behavior. So, we conjecture that, under certain conditions, the abrupt changes, delays, and noises as perturbations of a system do not modify certain properties such as controllability. In this regard, we prove the interior S∗-controllability of the semilinear stochastic heat equation with impulses and delay on the state variable, and this is done by using new techniques avoiding fixed point theorems employed by Bashirov et al.
1. Introduction
The term white-noise is denoted by , where m is a Gaussian process m = {(t, A) : t ∈ [0, τ], A ∈ ℬb(ℝd)} with zero mean and covariance given by (2). The noise m behaves as a Brownian motion with respect to the time variable, and it has a correlated spatial covariance.
There are many practical examples of impulsive control systems which are modeled by impulsive differential equations (for more information, see the monographs: Samoilenko and Perestyuk [6]; Franco and Nieto [7]; Sun and Zhang [8]; Lakshmikanthan, Bainov and Simeonov [9]; He and Yu [10]; Luo and Shen [11]). The controllability of impulsive evolution equations has been studied recently for several authors, but most them study the exact controllability only (to mention, Radhakrishnan and Balachandran [12]; Chalishajar [13]; Selvi and Mallika [14]). To our knowledge, there are a few works on approximate controllability of impulsive semilinear evolution equations (to mention, Chen and Li [15] and Sakthivel and Anandhi [16]). Recently, in the study of Carrasco, Leiva, Sanchez, and Tineo [17]; Leiva [1]; Leiva and Merentes [18], the approximate controllability of semilinear evolution equations with impulses has been studied applying Rothe’s fixed point theorem. Contrained controllability of finite-dimensional semilinear systems with delayed controls has been studied by Klamka [19, 20] where the author gives sufficient conditions for contrained local relative controllability applying a generalized open mapping theorem. Also, Klamka [21] gave necessary and sufficient conditions for different kinds of stochastic relative controllability in a given time interval which are proved for stochastic finite-dimensional linear systems with multiple delays in control.
The existence of solutions for impulsive evolution equations with delays has been studied by Hernandez, Sakthivel, and Tamaka [22]; Abada, Benchohra, and Hammouche [23]; Shikharchan and Baburao [24] and Chang [25, 26]. Besides, impulsive and stochastic effects appear in real-life systems. Moreover, a lot of dynamical systems have structure variables subject to stochastic abrupt changes, which may result from sudden phenomena such as stochastic failures and repair of components, quick environmental changes, and changes in the interconnections of subsystems (see Mao [27]). In the stochastic context, we can mention some papers related to impulsive and delay stochastic systems: Lijuan, Junping, and Jitao [28]; Sakthivel [16]; Sukavanam and Kumar [29]; Parthasarathy and Sathya [30].
The exact and approximate controllability is known for determinist systems; but the exact controllability was introduced as a concept for linear finite-dimensional systems by Kalman in the 50s. Nevertheless, the extension of this concept to infinite dimensional systems is too strong. Therefore, the approximate controllability was introduced as a weakened version of the exact controllability. However, the exact and approximate controllability cannot be a property of stochastic systems, and this needs to be a weaker concept than the approximate controllability concepts in order to extend them to the stochastic systems. Then, the concept of the S-controllability is introduced. A control system is S-controllable, if given an arbitrary ϵ > 0, it is possible to steer from the point z0 to within a distance from all points in the state space Z at time τ with probability close to one. The approximate controllability and S-controllability concepts are equivalent for the linear system but are different for nonlinear stochastic systems. This concept and generalization are defined in Bashirov et al. [5, 31]. In this context, we used the S∗-controllability which is a weaker version of S-controllability.
The main objective of this article is to prove the interior S∗-controllability of the semilinear stochastic heat equation with impulses, delay, and multiplicative noises (1) simultaneously, under appropriate conditions presented above. For this, we apply the new technique presented in Bashirov et al. [3, 4, 31, 32]. In the literature, S-controllability for such systems, only a few works such as Bashirov and an article by Sukavanam and Kumar [29], has been reported.
2. Preliminaries
In this section, we introduce notations, definitions, and preliminaries which are used to write (1) as an abstract differential equation.
Let Z, U, and K be separable Hilbert spaces and (Ω, ℱ, P) be a complete probability space with a probability measure P on Ω. Let {m(t), t ∈ [0, τ]} be a Wiener processes with values in K and covariance nonnegative operator Q ∈ L(K) (L(K) is the space of bounded linear operators on K). If the control system is stochastic, we denote by the smallest σ-field generated by {m(s) : 0 ≤ s ≤ τ}. We assume that there exists a complete orthonormal set {ξn, n = 1,2, …, } in K and a bounded sequence of nonnegative real numbers ρn such that Qξn = ρnξn with . Let βn(t), n = 1,2, …, be a sequence of real-valued one-dimensional standard Brownian motions mutually independent over (Ω, ℱ, P) such that .
We consider the function zt(x) : [−r, 0]⟶ℝ defined by zt(x)(s) = z(t + s, x), −r ≤ s ≤ 0 with r > 0 being the delay. Therefore, the initial condition ϕ(s, x) can be written as z0 = z0(x)(s) = ϕ(s, x), s ∈ [−r, 0], x ∈ Γ.
Definition 1. A stochastic control system is said to be S-controllable if
3. Abstract Formulation of the Problem
- (i)
For all z ∈ D(A), we have
-
where 〈⋅, ⋅〉 is the inner product in Z, {ϕj,k} is a complete orthonormal set of eigenvectors of A, and
-
So, {Ej} is a family of complete orthogonal projections in Z and .
- (ii)
−A generates an analytic semigroup {T(t)} given by
-
Therefore, system (1) can be written as abstract functional differential equations with impulses and noses (see Acosta-Leiva [33].
-
where , U = Z = K = L2(Γ), Bv : U⟶Z, Bθu = 1θu is a bounded linear operator, zt ∈ C([−r, 0]; Z) and is defined by zt(s) = z(t + s), −r ≤ s ≤ 0, ϕ ∈ C, and the operators , fe : [0, τ] × C × U⟶Z, are defined by
Proposition 1. Under condition (3) the function fe and ge satisfies
4. Approximate Controllability of the Linear Heat Equation
Definition 3. The stochastic linear system (20) is said to be approximately controllable on [0, τ] if for every initial state z0 ∈ ℱ0 and final state z1 ∈ L2(Ω, ℱτ, Z) and any ϵ > 0 there exists a control , Z = U = L2(Γ), such that the mild solution of (20) z(⋅) corresponding to u verifies
It is known that approximately controllability of the stochastic linear system (20) and deterministic linear system (22) for linear infinite dimensional systems are equivalent (see Mahmudov [34]). Now, we define the following operator.
Definition 4. (see [33]). For system (22), we define the following concept: the controllability maps Gτδ : L2([τ − δ, τ], U)⟶Z, Gδ : L2([0, δ], U)⟶Z defined by
The adjoint of these operators , are given by
The controllability operators Qδ : Z⟶Z are given by
Qτδ : Z⟶Z is defined by
The following lemma holds in general for a linear-bounded operator G : W⟶Z between Hilbert spaces W and Z(see Bashirov et al. [5]; Curtain and Pritchard [35]; Curtain and Zwart [36] and Leiva et al. [37]).
Lemma 1. The following statements are equivalent to the approximate controllability of the linear system (20) on [τ − δ, τ].
- (a)
- (b)
- (c)
〈Qτδz, z〉 > 0, z ≠ 0 in Z
- (d)
Remark 1. Lemma 1 implies that, for all z ∈ Z, we have
So, limα⟶0Gτδuα = z and the error Eτδz of this approximation is given by the formula:
Lemma 2. Qτδ > 0 if and only if linear system (22) is approximately controllable on [τ − δ, τ]. Moreover, given an initial state y0 ∈ Z and a final state z1, we can find a sequence of controls , where
5. S ∗-Controllability of the Semilinear Stochastic System
Proposition 2 (see [37].)If , then
Now, we are ready to present and prove the main result of this paper, the S∗-controllability of the semilinear heat equation with impulses, delay, and multiplicative noise.
Theorem 1. Under condition (3), the semilinear heat equations with impulses, delays, and multiplicative noise (1) is S∗-controllable on [0, τ].
Proof. Given ϕ ∈ C, a final state z1 ∈ Z, and ϵ > 0, we want to find a sequence of control steering the system from ϕ(0) to an ϵ-neighborhood of z1 ∈ Z on time τ in probability. Precisely, for 0 < δ < min{τ − tp, r} = σ < τ, there exists control such that the corresponding solution of (39) satisfies
Consider any process control and the corresponding solution of the initial value problem (39). For α ∈ (0,1], we define the control as
Now, since 0 < δ < τ − tp, the corresponding solution of the initial value problem (39) at time τ can be written as follows:
Therefore,
Hence,
Thus,
Also, the corresponding mild solution yδ,α(t) = y(t, τ − δ, z(τ − δ), uα) of the initial value problem of linear solution (22) at time τ is given by
Since z(τ − δ) is -measurable, and also yδ,α(τ) is -measurable, it is measurable with respect to the smaller σ field . On the other hand, we have that
Taking conditional expectation with respect to and using the fact that the term
Therefore, putting M = sup0≤t≤τ‖T(t)‖ and applying Jensen’ inequality, we have that
If we take 0 < δ < r and τ − δ < s < τ, then s − r < τ − r < τ − δ and zδ,α(s − r) = z(s − r). So, we obtain the following estimate:
Hence,
From equation (51), Lemma 1(d), and Proposition 2, we get that
Then, ‖yδ,α(τ) − z1‖ is dominated by an integrable random variable. Consequently, for every 0 < δ < τ,
Therefore, for fixed 0 < σ < τ, we can choose 0 < δn < σ such that
There exists αn > 0 such that
Then, there exists a sequence of controls such that
Since mean square convergence implies convergence in probability, we obtain
This completes the proof of the theorem.
6. Conclusions
In this article the approximate S∗-controllability was proved for the stochastic semilinear heat equation with impulse, delay, and multiplicative noise. For this, we avoid the method of fixed point theorems by applying a new alternative method due to Bashirov et al. This technique can be used to prove the S∗-controllability of the stochastic Benjamin Bona Mohany equation with impulses and delays, for the stochastic strongly damped wave equation under influence of impulses and delays and stochastic partial differential equations modelling the structural damped vibrations of a string or beam under the influence of impulses and delays.
Conflicts of Interest
The authors declare that they have no conflicts of interest.
Open Research
Data Availability
The data used in the research to support the findings of this study are purely Bibliographic and from scientific publications, which are included in the article with their respective citations.