Abstract
A nonlinear wave equation of Kirchhoff type with memory condition at the boundary in a bounded domain is considered. We establish a general decay result which includes the usual exponential and polynomial decay rates. Furthermore, our results allow certain relaxation functions which are not necessarily of exponential and polynomial decay. This improves earlier results in the literature.
MSC: 35L05; 35L70; 35L75; 74D10.
Keywords:
general decay; wave equation; relaxation; memory type; Kirchhoff type; nondissipative1 Introduction
In this article, we study the asymptotic behavior of the energy function related to a nonlinear wave equation of Kirchhoff type subject to memory condition at the boundary as follows:
where Ω is a bounded domain with smooth boundary ∂Ω = Γ_{0 }∪ Γ_{1}. The partition Γ_{0 }and Γ_{1 }are closed and disjoint, with meas(Γ_{0}) > 0, ν represents the unit normal vector directed towards the exterior of Ω, u is the transverse displacement, and g is the relaxation function considered positive and nonincreasing belonging to W^{1,2 }(Ω).
From the physical point of view, we know that the memory effect described in integral equation (1.3) can be caused by the interaction with another viscoelastic element. In fact, the boundary condition (1.3) signifies that Ω is composed of a material which is clamped in a rigid body in the portion Γ_{0 }of its boundary and is clamped in a body with viscoelastic properties in the portion of Γ_{1}.
When Γ_{1 }= ϕ, problem (1.1) has its origin in describing the nonlinear vibrations of an elastic string. More precisely, we have
for 0 < × < L, t ≥ 0; where u is the lateral deflection, x the space coordinate, t the time, E the Young modulus, ρ the mass density, h the cross section area, L the length, p_{0 }the initial axial tension and f the external force. Kirchhoff [1] was the first one who introduced (1.5) to study the oscillations of stretched strings and plates, so that (1.5) is called the wave equation of Kirchhoff type after him. In this direction, problem (1.1) with ∂Ω = Γ_{0 }and l(t) = 0 has been investigated by many authors in recent years, and many results concerning existence, nonexistence and asymptotic behavior have been established, see [213].
On the other hand, regarding the viscoelastic wave equations with memory term acting in the boundary or in the domain, there are numerous results related to asymptotic behavior of solutions. For example, in the case where M(s) = 1, Cavalcanti et al. [14] investigated the existence and uniform decay of strong solutions of wave equation (1.1) with a nonlinear boundary damping of memory type and a nonlinear boundary source when l(t) = 0. Cavalcanti and Guesmia [15] considered the following system:
where Ω is a bounded domain with smooth boundary ∂Ω = Γ_{0 }∪ Γ_{1}. They obtained the general decay result which depends on the relaxation function g. In particular, if the relaxation function g decays exponentially (or polynomially), then the solution also decays exponentially (or polynomially) and with the same decay rate. Moreover, when u_{0 }= 0 on Γ_{1}, they obtained exponential or polynomial decay of solutions, even if the relaxation function g does not converge to 0 at ∞. Later, Messaoudi and Soufyane [16] generalized this result to the case of a system of Timoshenko type. They established general decay rate results, from which the usual exponential and polynomial decay rates are only special cases. Recently, Messaoudi and Soufyane [17] studied the following problem:
in a bounded domain with boundary conditions (1.7)(1.9). They improved the results of [15] by applying the multiplier techniques. Indeed, they obtained not only a general decay result, but their works also allowed certain relaxation functions which are not necessarily of exponential or polynomial decay. For other related works, we refer the reader to [1820] and references therein.
Conversely, in the case where M is not a constant function, Santos [21] considered
where μ(t) is a nonincreasing function satisfying μ(t) ≥ μ_{0 }> 0. By denoting k the resolvent kernel of g', he showed that the solution decays exponentially (or polynomially) to zero provided k decays exponentially (or polynomially) to zero. Later on, Santos et al. [22] generalized this result to a nonlinear ndimensional equation of Kirchhoff type of the form
in a bounded domain with boundary conditions (1.2)(1.3). In that article, they proved that the energy decays with the same rate of decay of the relaxation function. This latter result improved an earlier one by Park et al. [23], where the authors considered (1.10) in a bounded domain with nonlinear boundary damping and memory term and M(s) = 1 + s and f = 0.
We note that stability of problems with the nonlinear term h(∇u) requires a careful treatment because we do not have any information about the influence
of the integral
In order to obtain our results, we consider system (1.1)(1.4), under some assumptions on a(x), l(t), M and f. Precisely, we state the general assumptions:
(A1) a(x): Ω → R^{+ }is a function.
(A2) f ∈ C^{1}(R) is a function and satisfies
where
d > 0 and
(A3) M is a C^{1 }function on [0, ∞) satisfying
Where
(A4) h : R^{n }→ R is a C^{1 }function such that ∇h is bounded and there exists β_{1 }> 0 such that
and l(t) is a positive and nonincreasing function.
The remainder of this article is organized as follows. In Section 2, we introduce some notations, present Lemma 2.1 to describe more general relations between the relaxation function g and the corresponding resolvent kernel k and state the existence result to system (1.1)(1.4). In Section 3, we give the proof of our main result Theorem 3.5.
2 Preliminaries
In this section, we introduce some notations and establish the existence of solutions
of the problem (1.1)(1.4). In what follows, let ·_{p }denote the usual L^{p }(Ω) norm
and set
Using Hölder's inequality, we observe that
Next, we shall use Equation 1.3 to estimate the boundary term
Assume the function k is the resolvent kernel of the relaxation function g, then
Applying Volterra's inverse operator yields
which implies that
where
Lemma 2.1. [15,17,22]If h : [0, ∞) → R^{+ }is continuous, then k is also a positive continuous function. Moreover,
(1) If there exists a positive constant c_{0 }such that
where γ : [0, ∞) → R^{+}, is a nonincreasing function satisfying, for some positive constant ε < 1,
Then, k satisfies
(2) Suppose that
for c_{0 }< p  1. Then, there exists a positive constant ε < 1 such that
where β > 0 is a constant.
Based on this lemma, we will use (2.5) instead of (1.3), i.e., we can consider system (1.1)(1.4) as follows:
We notice that, due to the condition (1.2), the solution of system (1.1)(1.4) must belong to the following space:
which endowed with the norm ∇·_{2 }is a Hilbert space. Now, we are ready to give the wellposedness of system (1.1)(1.4).
Theorem 2.2. Let k ∈ W^{2,1 }(R^{+}) ∩ W^{1,∞ }(R^{+}), (u_{0}, u_{1}) ∈ (H^{2 }(Ω) ∩ V)^{2 }and satisfy the compatibility condition
Assume further that (A1)(A4) hold. Then, there exists a unique solution u of system (1.1)(1.4) such that
Proof. Using the Galerkin method and procedures similar to that of [22,28], we can obtain the result. □
3 Decay of solutions
In this section, we study the asymptotic behavior of the solutions of system (1.1)(1.4) when the resolvent kernel k satisfies
where γ : [0, ∞) → R^{+ }is a function satisfying the following condition:
To get our result, we further assume that
Let x_{0 }be a fixed point in R^{n}. Set
and partition the boundary ∂Ω into two sets
Define the firstorder energy function of system (1.1)(1.4) by
The following lemma is associated with the property of the convolution operator, which is used to estimate the energy identity.
Lemma 3.1. If g, ϕ ∈ C^{1}(R^{+}), then
Proof. Our conclusion is followed by differentiating the term g ○ ϕ. □
Lemma 3.2. Under the assumptions of (A1)(A4), the energy function E(t) satisfies
Proof. Multiplying Equation 1.1 by u_{t}, and integrating by parts over Ω, we get
Exploiting (2.5), (3.6) and the definition of E(t) by (3.5), we have
Then, using Hölder's inequality and Young's inequality, the inequality (3.7) is obtained. □
Next, we construct a Lyapunov functional which is equivalent to E(t). To do so, for N > 0 large enough, let
where
for 0 < θ < 1.
For the purpose of achieving our main result, we need the following lemmas.
Lemma 3.3. There exist two positive constants α_{1 }and α_{2 }such that the relation
holds for all t ≥ 0.
Proof. From (3.9) and using Young's inequality, we get
where we have used the fact that
due to
Thus, from (3.8), we deduce that
Hence, selecting
there exist two positive constants α_{1 }and α_{2 }such that the relation
holds. □
Lemma 3.4. Let (A1)(A4) and (3.1)(3.3) hold, with β_{1 }(given by (A4)) small enough and
Then, for some t_{0 }large enough, the functional L(t) verifies, along the solution u of (1.1)(1.4),
for all t ≥ t_{0}, where α = min {2θ, 1  θ} and c_{i }are positive constants given in the proof, i = 4, 5.
Proof. First, we are going to estimate the derivative of ψ(t). From (3.9) and using Equation 1.1, we have
Performing integration by parts and using Young's inequality, we obtain
where ε > 0, c_{ε }and c_{0 }are some positive constants. In the following, we will estimate the last two terms on the righthand side of (3.15). It follows from (1.13), Hölder's inequality, (3.11), (3.3) and (3.10) that
where
A substitution of (3.16)(3.17) into (3.15), we obtain
Now, we analyze the boundary term on the righthand side of (3.18). Applying Young's inequality and M(λ) ≥ m_{0 }> 0 by (1.12), we have, for ε_{1 }> 0,
where
Thus, (3.18) becomes
By rewriting the boundary condition (2.5) as
and, then, combining (3.7) and (3.20), we deduce that
Similarly as in deriving (3.16), we note that
where
At this point, we choose
Once ε = ε_{1 }is fixed (hence c_{ε }and
at the same time. Then, from the properties of k(t) by (3.1) and noting that
Utilizing the inequality
which together with (3.19) and (3.10) infers that
where α = min{2θ, 1  θ}. Besides, we note that there exists t_{0 }large enough satisfying
because of lim_{t→∞} k(t) = 0 by (3.13). Therefore, taking β_{1 }small enough such that
then,
for all t ≥ t_{0}, where c_{i }are positive constants, i = 4, 5. This completes the proof. □
Theorem 3.5. Given that (u_{0}, u_{1}) ∈ (H^{2 }(Ω) ∩ V)^{2}, assume that (A1)(A4), (3.1)(3.3) and (3.13)hold, with β_{1 }(given by (A4)) small enough. Assume further that
Then, for some t_{0 }large enough, we have, ∀t ≥ t_{0},
otherwise (if u_{0 }≠ 0 on Γ_{1}),
where a_{1 }is a fixed positive constant and cis a generic positive constant.
Proof. Multiplying (3.25) by γ(t) and exploiting (3.26), (3.1) and (3.7), we derive that
where c_{6 }= c_{4}γ(0) + c_{5 }and
where
which is equivalent to E(t) due to Lemma 3.3 and γ(t) is nonincreasing by (3.2). In addition to (3.24), we further require
then, we have
where a_{1 }is a positive constant.
Case I: If u_{0 }= 0 on Γ_{1}, then (3.30) reduces to
Integrating the above inequality over (t_{0}, t) to get
Then, using the fact F_{1}(t) is equivalent to E(t), we obtain, for some positive constant c,
Thus, (3.27) is proved.
Case II: If u_{0 }≠ 0 on Γ_{1}, then (3.30) gives
where
An integration over (t_{0}, t) yields
Again using the fact F_{1}(t) is equivalent to E(t), we obtain, for some positive constant c,
This completes the proof of Theorem 3.5. □
4 Conclusion and suggestions
Santos et al. [22] considered problem (1.1)(1.4) with a = 1 and without a function of the gradient term. They showed the solution decays exponentially (or polynomially) to zero provided the kernel decays exponentially (or polynomially) to zero. Recently, Messaoudi and Soufyane in 2010 [17] considered a semilinear wave equation, in a bounded domain, where the memorytype damping is acting on the boundary. They established a general decay result, from which the usual exponential and polynomial decay rate are only special cases. Motivated by this, we intended to investigate the decay properties of problem (1.1)(1.4) using the work of Messaaoudi and Soufyane [17]. Since stability of problems with the nonlinear term h(∇u) requires a careful treatment, it is interesting to investigate whether we still have the similar general decay result as that of [16] in the presence of a function of the gradient term. This is our motivation to consider problem (1.1)(1.4). And, this problem is not considered before.
By adopting and modifying the method proposed by Messaoudi and Soufyane in 2010 [17], we establish a general decay result, from which the usual exponential and polynomial
decay rate are only special cases. Further, our result allows certain kernels which
are not necessarily of exponential or polynomial decay. In this way, we improved the
results of Santos et al. [22], in which they considered problem (1.1)(1.4) with a = 1 and in the absence of l(t)h (∇u). Moreover, we note that our result also holds for problem (1.1)(1.4) with a = 1 and l(t) = 0 and without imposing strong damping term, thus our result improves the one of
Bae et al. [27]. More precisely, the estimate (3.27) and (3.28) generalizes the exponential and polynomial
decay result given in [22,27]. Indeed, we obtain exponential decay for γ(t) = c and polynomial decay for γ(t) = c(1 + t)^{1}, where c is a positive constant. Additionally, as in [17], our result allows kernels which satisfy k″(t) ≥ c (k′)^{1+q}, for 0 < q < 1 instead of the usual assumption
It is clear that
Though we consider the conditions on the term involving the gradient are too restrictive and we combine some known ideas to obtain our result, our findings extend those decay results in [22,27] and these findings are interesting to those with closely concerns. For future work, we will consider not necessarily decreasing kernels and relax the condition of h(∇u).
Competing interests
The author declare that they have no competing interests.
Acknowledgements
The author would like to thank the anonymous referees for their valuable and constructive suggestions which improve this work.
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