Volume 2012, Issue 1 936140
Research Article
Open Access

Asymptotic Behavior for a Nondissipative and Nonlinear System of the Kirchhoff Viscoelastic Type

Nasser-Eddine Tatar

Corresponding Author

Nasser-Eddine Tatar

Department of Mathematics & Statistics, King Fahd University of Petroleum & Minerals, Dhahran 31261, Saudi Arabia kfupm.edu.sa

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First published: 16 August 2012
Academic Editor: Yongkun Li

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

We will consider the following wave equation with a viscoelastic damping term:
()
where Ω is a bounded domain in Rn with smooth boundary Γ = Ω and pi, qj > 0,   i = 1, …, m,  j = 1, …, k. The functions u0(x) and u1(x) are given initial data, and the (nonnegative) functions aj(t),  bi(t), and h(t) are at least absolutely continuous and will be specified later on. This problem arises in viscoelasticity where it has been shown by experiments that when subject to sudden changes, the viscoelastic response not only does depend on the current state of stress but also on all past states of stress. This gives rise to the integral term called the memory term. One may find a rich literature in this regard (with or without the Kirchhoff terms) treating mainly the stabilization of such systems for different classes of functions h. We refer the reader to [125] and the references therein. For problems of the Kirchhoff type, one can consult [2635] and in particular [3646] where the equations are supplemented by a nonlinear source. Several questions, such as well-posedness and asymptotic behavior, have been discussed in these references, to cite but a few.

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

()
for T small enough.

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

In this section we define the different functionals we will work with. We prove an equivalence result between two functionals. Further, some useful lemmas are presented. We define the (classical) energy by
()
where ∥·∥p denotes the norm in Lp(Ω). Then by  (1.1)  it is easy to see that for t ≥ 0
()
The first term in the right-hand side of (2.2) may be written as the derivative of some expression; namely,
()
where
()
Therefore, if we modify E(t) to
()
we obtain for t ≥ 0
()
Assuming that
()
makes (t) a nonnegative functional. The following functionals
()
are standard and will be used here. The next ones have been introduced by the present author in [24]
()
where
()
and γ(t) and ξ(t) are two nonnegative functions which will be precised later (see (H2), (H3)). The functional
()
for some λi > 0,   i = 1,2, 3,4, to be determined is equivalent to (t) + Φ3(t) + Φ4(t).

Proposition 2.1. There exist ρi > 0,   i = 1,2 such that

()
for all t ≥ 0 and small λi,   i = 1,2.

Proof. By the inequalities

()
where Cp is the Poincaré constant, we have
()
On the other hand,
()
Therefore, ρ1[(t) + Φ3(t) + Φ4(t)] ≤ L(t) ≤ ρ2[(t) + Φ3(t) + Φ4(t)] for some constant ρi > 0,   i = 1,2 and small λi,   i = 1,2 such that λ1 < min {1, (1 − κ)/Cp} and λ2 < min {1/Cpκ, 1 − λ1}.

The identity to follow is easy to justify and is helpful to prove our result.

Lemma 2.2. One has for hC(0, ) and vC((0, ); L2(Ω))

()

The next lemma is crucial in estimating (partially) our nonlinear terms. It can be found in [47].

Let IR, and let g1, g2 : IR∖{0}. We write g1g2 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 g1g2 ∝ ⋯∝gn in (0, ), then the inequality

()
implies that
()
where c0(t): = sup 0≤sta(s),
()
and β0 is chosen so that the functions cj(t),   j = 1, …, n are defined for αt < β0.

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

()
for .

3. Asymptotic Behavior

In this section we state and prove our result. To this end we need some notation. For every measurable set 𝒜R+, we define the probability measure by
()
The nondecreasingness set and the non-decreasingness rate of h are defined by
()
()
respectively.
The following assumptions on the kernel h(t) will be adopted.
  • (H1) h(t) ≥ 0 for all t ≥ 0 and .

  • (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.

  • (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 t the set t : = ∩[0, t].

Lemma 3.1. One has for tt* and δi > 0,   i = 1, …, 5

()
where BV[h] is the total variation of h.

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

()
or
()
Therefore,
()
For all measurable sets 𝒜 and 𝒬 such that 𝒜 = R+𝒬, it is clear that
()
For δ1 > 0, the first term in the right-hand side of (3.8) satisfies
()
and the third one fulfills
()

Back to (3.8) we may write

()
The last term in the right-hand side of (3.7) will be estimated as follows:
()
For the fourth term in (3.7), it holds that
()
Moreover, from Lemma 2.4, for p > 0 if n = 1,2 and 0 < p < 2/(n − 2) if n ≥ 3, we find
()
The definition of (t) in (2.5) allows us to write
()

Gathering all the relations (3.11)–(3.15) together with (3.7), we obtain for tt*

()

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 pq and A(t)↔B(t) in the proof following it. The case p = q is easier.

We will make use of the following hypotheses for some positive constants A,   B,   U, and V to be determined.
  • (A) a(t) is a continuously differentiable function such that a(t) < Aa(t),   t ≥ 0.

  • (B) b(t) is a continuously differentiable function such that b(t) < Bb(t),   t ≥ 0.

  • (C) p > 0 if n = 1,2 and 0 < p < 2/(n − 2) if n ≥ 3.

  • (D) .

  • (E) .

Theorem 3.2. Assume that the hypotheses (H1)–(H3), (A)–(C) hold and h < 1/4. If , then, for global solutions and small , there exist T1 > 0 and U > 0 such that L(t) > U,   tT1 or

()
for some positive constants M1 and ν1 as long as (D) holds. If , then there exist T2 > 0 and V > 0 such that L(t) > V,   tT2 or
()
for some positive constants M2 and ν2 as long as (E) holds.

Proof. A differentiation of Φ1(t) with respect to t along trajectories of (1.1) gives

()
and Lemma 2.2 implies
()
Next, a differentiation of Φ3(t) and Φ4(t) yields
()

Taking into account Lemma 3.1 and the relations (2.6), (3.20)-(3.21), we see that

()
Next, as in [17], we introduce the sets
()
and observe that
()
where 𝒩h is the null set where h is not defined and 𝒬h is as in (3.2). Furthermore, if we denote 𝒬n : = R+𝒜n, then because 𝒬n+1𝒬n for all n and . Moreover, we designate by the sets
()
In (3.22), we take and . Choosing λ1 = (h*ε)λ2, it is clear that
()
for small ε and δ2, large n and t*, if . We deduce that
()
Furthermore, if , then
()
with
()
and a small β > 0. Pick
()
and Hγ(0) such that
()
Note that this is possible if t* is so large that h* > 7κ/(8 − κ) even though
()

Taking the relations (3.22)–(3.30) into account and selecting λ2 < δ3/CpBV[h] so that

()
and small enough so that
()
we find for δ3 = ε/2, large δ4, small Ψγ(0), and tt*
()
for some positive constant C1. Take small, and
()
(i.e., A = 2(q + 1)(λ1α) for some 0 < α < λ1) and
()
(i.e., B = (p + 2)(λ1β) for some 0 < β < λ1) to derive that
()
for some positive constant C2.

If lim tη(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

()
where
()
If there exists a such that , where , then from (3.39)
()
and it follows that for tT
()
with . Now we apply Lemma 2.3 to get
()
where and . If, in addition, , then is uniformly bounded by a positive constant C4. Thus
()
and by continuity (3.44) holds for all t ≥ 0.

If lim tη(t) = 0, then for any C > 0 there exists a such that η(t) ≤ C for . Therefore,

()
for some C5 > 0. The previous argument carries out with replaced by .

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)(λ1α)a(t) and b(t) < (p + 2)(λ1β)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.

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