Approximate Controllability of a Semilinear Heat Equation
Abstract
We apply Rothe’s type fixed point theorem to prove the interior approximate controllability of the following semilinear heat equation: zt(t, x) = Δz(t, x) + 1ωu(t, x) + f(t, z(t, x), u(t, x)) in (0, τ] × Ω, z = 0, on (0, τ) × ∂Ω, z(0, x) = z0(x), x ∈ Ω , where Ω is a bounded domain in ℝN (N ≥ 1), z0 ∈ L2(Ω), ω is an open nonempty subset of Ω, 1ω denotes the characteristic function of the set ω, the distributed control u belongs to L2(0, τ; L2(Ω)), and the nonlinear function f : [0, τ] × ℝ × ℝ → ℝ is smooth enough, and there are a, b, c ∈ ℝ, R > 0 and 1/2 ≤ β < 1 such that |f(t, z, u) − az | ≤ c | u|β + b, for all u, z ∈ , |u | , |z | ≥ R. Under this condition, we prove the following statement: for all open nonempty subset ω of Ω, the system is approximately controllable on [0, τ]. Moreover, we could exhibit a sequence of controls steering the nonlinear system from an initial state z0 to an ϵ neighborhood of the final state z1 at time τ > 0.
1. Introduction
Definition 1 (approximate controllability). The system (1) is said to be approximately controllable on [0, τ] if for every z0, z1 ∈ Z = U = L2(Ω), ɛ > 0, there exists u ∈ L2(0, τ; U) such that the solution z(t) of (1) corresponding to u verifies

Remark 2. It is clear that exact controllability of the system (1) implies approximate controllability, null controllability, and controllability to trajectories of the system. But it is well known (see [1]) that due to the diffusion effect or the compactness of the semigroup generated by −Δ, the heat equation can never be exactly controllable. We observe also that in the linear case, controllability to trajectories and null controllability are equivalent. Nevertheless, the approximate controllability and the null controllability are in general independent. Therefore, in this paper, we shall concentrate only on the study of the approximate controllability of the system (1).
Now, we shall describe the strategy of this work.
Proposition 3. Let (X, Σ, μ) be a measure space with μ(X) < ∞ and 1 ≤ q < r < ∞. Then, Lr(μ) ⊂ Lq(μ) and
Proof. The proof of this proposition follows from Theorem I.V.6 from [12] by putting p = r/q > 1 and considering the relation
Theorem 4 (Rothe’s theorem [13, page 129]). Let E(τ) be a Hausdorff topological vector space. Let B ⊂ E be a closed convex subset such that the zero of E is contained in the interior of B.
Let Φ : B → E be a continuous mapping with Φ(B) relatively compact in E and Φ(∂B) ⊂ B.
Then, there is a point x* ∈ B such that Φ(x*) = x*.
The technique we use here to prove the approximate controllability of the linear part of (10) is based on the classical unique continuation for elliptic equations (see [14]) and the following lemma.
Lemma 5 (see Lemma 3.14 from [15], page 62.)Let {αj} j≥1 and {βi,j : i = 1,2, …, m} j≥1 be two sequences of real numbers such that α1 > α2 > α3⋯. Then,
2. Abstract Formulation of the Problem
In this section, we choose a Hilbert space where system (1) can be written as an abstract differential equation; to this end, we consider the following results appearing in [15, page 46], [16, page 335], and [17, page 147].
- (i)
There exists a complete orthonormal set {ϕj,k} of eigenvectors of A = −Δ.
- (ii)
For all z ∈ D(A), we have
() -
where 〈·, ·〉 is the inner product in Z and
() -
So, {Ej} is a family of complete orthogonal projections in Z and , z ∈ Z.
- (iii)
−A generates an analytic semigroup {T(t)} given by
()
Proposition 6. Under condition (12), the function ge : [0, τ] × Z × U → Z defined by ge(t, z, u)(x) = g(t, z(x), u(x)), for all x ∈ Ω, satisfies for all u, z ∈ Z = L2(Ω):
3. Interior Controllability of the Linear Equation
Definition 7. For system (21), we define the following concept: the controllability map (for τ > 0) Ga : L2(0, τ; U) → Z is given by
The following lemma holds in general for a linear bounded operator G : W → Z between Hilbert spaces W and Z.
Lemma 8 (see [11], [15], [18].)Equation (21) is approximately controllable on [0, τ] if and only if one of the following statements holds.
- (a)
.
- (b)
.
- (c)
, z ≠ 0 in Z.
- (d)
.
- (e)
, for all t ∈ [0, τ], ⇒z = 0.
- (f)
For all z ∈ Z , we have , where
()
So, lim α→0Gauα = z and the error Eαz of this approximation is given by
Remark 9. Lemma 8 implies that the family of linear operators Γα : Z → L2(0, τ; U), defined for 0 < α ≤ 1 by
is an approximate inverse for the right of the operator Ga in the sense that
Proposition 10 (see [7].)If , then
Remark 11. The proof of the following theorem follows from foregoing characterization of dense range linear operators and the classical unique continuation for elliptic equations (see [14]), and it is similar to the one given in Theorem 4.1 in [6].
4. Controllability of the Semilinear System
Definition 13. For the system (22), we define the following concept: the nonlinear controllability map (for τ > 0) Gg : L2(0, τ; U) → Z is given by
The following lemma is trivial.
Lemma 14. Equation (22) is approximately controllable on [0, τ] if and only if .
Definition 15. The following equation shall be called the controllability equation associated with the nonlinear equation (22):
Now, we are ready to present and prove the main result of this paper, which is the interior approximate controllability of the semilinear nD heat equation (1)
Theorem 16. The system (22) is approximately controllable on [0, τ]. Moreover, a sequence of controls steering the system (22) from initial state z0 to an ϵ-neighborhood of the final state z1 at time τ > 0 is given by
Proof. For each z ∈ Z fixed, we shall consider the following family of nonlinear operators Kα : L2(0, τ; U) → L2(0, τ; U) given by
Moreover,
In fact, for the purpose of contradiction, let us assume the contrary. Then, there exists a subsequence such that
5. Final Remark
Our technique is simple and can be applied to those systems involving compact semigroups like some control system governed by diffusion processes. For example, the Benjamin-Bona-Mahony equation, the strongly damped wave equations, beam equations, and so forth.
Example 17. The original Benjamin-Bona-Mahony equation is a nonlinear one in [21] the authors proved the approximate controllability of the linear part of this equation, which is the fundamental base for the study of the controllability of the nonlinear BBM equation. So, our next work is concerned on the controllability of nonlinear BBM equation:
Example 18. We believe that this technique can be applied to prove the interior controllability of the strongly damped wave equation with Dirichlet boundary conditions:
Example 19. Another example where this technique may be applied is partial differential equations modeling the structural damped vibrations of a string or a beam:
Theorem 20. If vectors B*ϕj,k are linearly independent in Z, then the system (69) is approximately controllable on [0, τ].
Acknowledgments
This work has been supported by CDCHT-ULA-C-1796-12-05-AA and BCV.