Asymptotic Behavior for a Nondissipative and Nonlinear System of the Kirchhoff Viscoelastic Type
Abstract
A wave equation of the Kirchhoff type with several nonlinearities is stabilized by a viscoelastic damping. We consider the case of nonconstant (and unbounded) coefficients. This is a nondissipative case, and as a consequence the nonlinear terms cannot be estimated in the usual manner by the initial energy. We suggest a way to get around this difficulty. It is proved that if the solution enters a certain region, which we determine, then it will be attracted exponentially by the equilibrium.
1. Introduction
As is clear from the equation in (1.1), we consider here several nonlinearities and the relaxation function is not necessarily decreasing or even nonincreasing. These issues are important but do not constitute the main contribution in the present paper. In case that aj(t) and bi(t) are not nonincreasing, then we are in a nondissipative situation. This is the case also when the relaxation function oscillates (in case aj(t), bi(t) are nonincreasing). Our argument here is simple and flexible. It relies on a Gronwall-type inequality involving several nonlinearities. We prove that there exists a sufficiently large T > 0 and a constant U after which (the modified energy of) global solutions are bounded below by U or decay to zero exponentially. We were not able to find conditions directly on the initial data because the Gronwall inequality is applicable only after some large values of time.
For simplicity we shall consider the simpler case p1 = p, pi = 0, b1 = b, bi = 0, i = 2, …, m and q1 = q, qj = 0, a1 = a, aj = 0, j = 2, …, k.
The local existence and uniqueness may be found in [36, 37].
Theorem 1.1. Assume that and h(t) is a nonnegative summable kernel. If 0 < p < 2/(n − 2) when n ≥ 3 and p > 0 when n = 1,2, then there exists a unique solution u to problem (1.1) such that
The plan of the paper is as follows. In the next section we prepare some materials needed to prove our result. Section 3 is devoted to the statement and proof of our theorem.
2. Preliminaries
Proposition 2.1. There exist ρi > 0, i = 1,2 such that
Proof. By the inequalities
The identity to follow is easy to justify and is helpful to prove our result.
Lemma 2.2. One has for h ∈ C(0, ∞) and v ∈ C((0, ∞); L2(Ω))
The next lemma is crucial in estimating (partially) our nonlinear terms. It can be found in [47].
Let I ⊂ R, and let g1, g2 : I → R∖{0}. We write g1 ∝ g2 if g2/g1 is nondecreasing in I.
Lemma 2.3. Let a(t) be a positive continuous function in J : = [α, β), kj(t), j = 1, …, n are nonnegative continuous functions, gj(u), j = 1, …, n are nondecreasing continuous functions in R+, with gj(u) > 0 for u > 0, and u(t) is a nonnegative continuous functions in J. If g1 ∝ g2 ∝ ⋯∝gn in (0, ∞), then the inequality
Lemma 2.4. Assume that 2 ≤ q < +∞ if n = 1,2 or 2 ≤ q < 2n/(n − 2) if n ≥ 3. Then there exists a positive constant Ce = Ce(Ω, q) such that
3. Asymptotic Behavior
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(H1) h(t) ≥ 0 for all t ≥ 0 and .
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(H2) h is absolutely continuous and of bounded variation on (0, ∞) and h′(t) ≤ ξ(t) for some nonnegative summable function ξ(t) (=max {0, h′(t)} where h′(t) exists) and almost all t > 0.
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(H3) There exists a nondecreasing function γ(t) > 0 such that γ′(t)/γ(t) = η(t) is a nonincreasing function: and .
Note that a wide class of functions satisfies the assumption (H3). In particular, exponentially and polynomially (or power type) decaying functions are in this class.
Let t* > 0 be a number such that . We denote by ℬt the set ℬt : = ℬ∩[0, t].
Lemma 3.1. One has for t ≥ t* and δi > 0, i = 1, …, 5
Proof. This lemma is proved by a direct differentiation of Φ2(t) along solutions of (1.1) and estimation of the different terms in the obtained expression of the derivative. Indeed, we have
Back to (3.8) we may write
Gathering all the relations (3.11)–(3.15) together with (3.7), we obtain for t ≥ t*
In the following theorem we will assume that p < q just to fix ideas. The result is also valid for p > q. It suffices to interchange p↔q and A(t)↔B(t) in the proof following it. The case p = q is easier.
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(A) a(t) is a continuously differentiable function such that a′(t) < Aa(t), t ≥ 0.
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(B) b(t) is a continuously differentiable function such that b′(t) < Bb(t), t ≥ 0.
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(C) p > 0 if n = 1,2 and 0 < p < 2/(n − 2) if n ≥ 3.
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(D) .
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(E) .
Theorem 3.2. Assume that the hypotheses (H1)–(H3), (A)–(C) hold and ℛh < 1/4. If , then, for global solutions and small , there exist T1 > 0 and U > 0 such that L(t) > U, t ≥ T1 or
Proof. A differentiation of Φ1(t) with respect to t along trajectories of (1.1) gives
Taking into account Lemma 3.1 and the relations (2.6), (3.20)-(3.21), we see that
Taking the relations (3.22)–(3.30) into account and selecting λ2 < δ3/CpBV[h] so that
If lim t→∞η(t) ≠ 0, then there exist a and C3 > 0 such that η(t) ≥ C3 for . Thus, in virtue of Proposition 2.1, for C3 > 0, we have
If lim t→∞η(t) = 0, then for any C > 0 there exists a such that η(t) ≤ C for . Therefore,
In case that q < p, we reverse the roles of p and q in the argument above. The case p = q is clear.
Remark 3.3. The case where the derivative of the kernel does not approach zero on 𝒜 (as is the case, for instance, when h′ ≤ −Ch on 𝒜) is interesting. Indeed, the right-hand side in condition (3.34) will be replaced by C/4 with a possibly large constant C.
Remark 3.4. The argument clearly works for all kinds of kernels previously treated where derivatives cannot be positive or even take the value zero. In these cases there will be no need for the smallness conditions on the kernels. This work shows that derivatives may be positive (i.e., kernels may be increasing) on some “small” subintervals and open the door for (optimal) estimations and improvements of these sets.
Remark 3.5. The assumptions a′(t) < 2(q + 1)(λ1 − α)a(t) and b′(t) < (p + 2)(λ1 − β)b(t) may be relaxed to a′(t) < 2(q + 1)λ1a(t) and b′(t) < (p + 2)λ1b(t), respectively. In this case α = α(t) and β = β(t) would depend on t.
Remark 3.6. The assertion in Theorem 3.2 is an “alternative” statement. As a next step it would be nice to discuss the (sufficient conditions of) occurrence of each case in addition to the global existence.
Acknowledgment
The author is grateful for the financial support and the facilities provided by the King Fahd University of Petroleum and Minerals.