# A blow up result for viscoelastic equations with arbitrary positive initial energy

- Jie Ma
^{1}Email author, - Chunlai Mu
^{1}and - Rong Zeng
^{1}

**2011**:6

https://doi.org/10.1186/1687-2770-2011-6

© Ma et al; licensee Springer. 2011

**Received: **5 March 2011

**Accepted: **12 July 2011

**Published: **12 July 2011

## Abstract

## Keywords

## 1 Introduction

where Ω is a bounded domain of *R*^{
n
} with smooth boundary ∂Ω, *p* > 1, *q* > 1 and *g* is a positive function. The wave equations (1.1) appear in applications in various areas of mathematical physics (see [1]).

If the equations in (1.1) have not the viscoelastic term
, the equations are known as the wave equation. In this case, the equations have been extensively studied by many people. We observe that the wave equation subject to nonlinear boundary damping has been investigated by the authors Cavalcanti et al. [2, 3] and Vitillaro [4, 5]. It is important to mention other papers in connection with viscoelastic effects such as Aassila et al. [6, 7] and Cavalcanti et al. [8]. Furthermore, related to blow up of the solutions of equations with nonlinear damping and source terms acting in the domain we can cite the work of Alves and Cavalcanti [9], Cavalcanti and Domingos Cavalcanti [10]. As regards non-existence of a global solution, Levine [11] firstly showed that the solutions with negative initial energy are non-global for some abstract wave equation with linear damping. Later Levine and Serrin [12] studied blow-up of a class of more generalized abstract wave equations. Then Pucci and Serrin [13] claimed that the solution blows up in finite time with positive initial energy which is appropriately bounded. In [14] Levine and Todorova proved that there exist some initial data with arbitrary positive initial energy such that the corresponding solution to the wave equations blows up in finite time. Then Todorova and Vitillaro [15] improved the blow-up result above. However, they did not give a sufficient condition for the initial data such that the corresponding solution blows up in finite time with arbitrary positive initial energy. Recently, for problem (1.1) with *g* ≡ 0 and *m* = 1, Gazzalo and Squassina [16] established the condition for initial data with arbitrary positive initial energy such that the corresponding solution blows up in finite time. Zeng et al. [17] studied blowup of solutions for the Kirchhoff type equation with arbitrary positive initial energy.

*g*(

*s*) and

*a*(

*x*). At this point it is important to mention some papers in connection with viscoelastic effects, among them, Alves and Cavalcanti [9], Aassila et al. [7], Cavalcanti and Oquendo [19] and references therein. Then Messaoudi [20] obtained the global existence of solutions for the viscoelastic equation, at same time he also obtained a blow-up result with negative energy. Furthermore, he improved his blow-up result in [21]. Recently, Wang and Wang [22] investigated the following problem

and showed the global existence of the solutions if the initial data are small enough. Moreover, they derived decay estimate for the energy functional. In [23] Wang established the blow-up result for the above problem when the initial energy is high.

We next state some assumptions on *g*(*s*) and real numbers *p* > 1, *q* > 1.

for all *v* ∈ *C*^{1}([0, ∞)) and *t* > 0.

**Remark 1.1**. It is clear that *g*(*t*) = *εe* ^{
-t
} (0 < ε < 1) satisfies the assumptions (A1) and (A2).

Based on the method of Faedo-Galerkin and Banach contraction mapping principle, the local existence and uniqueness of the problem (1.2) have been established in [8, 18, 25, 26] as follows.

**Theorem 1.1**. Under the assumptions (A1)-(A3), let the initial data , (

*u*

_{1},

*v*

_{1}) ∈

*L*

^{2}(Ω) ×

*L*

^{2}(Ω). Then the problem (1.2) has a unique local solution

for the maximum existence time *T*, where *T* ∈ (0, ∞].

Our main blow-up result for the problem (1.2) with arbitrarily positive initial energy is stated as follows.

**Theorem 1.2**. Under the assumptions (A1)-(A3), if and the initial data and (

*u*

_{1},

*v*

_{1}) ∈

*L*

^{2}(Ω) ×

*L*

^{2}(Ω) satisfy

*χ*is the constant of the Poincaré's inequality on Ω, , energy functional

*E*(

*t*) and

*I*(

*u*,

*v*) are defined as

The rest of this paper is organized as follows. In Section 2, we introduce some lemmas needed for the proof of our main results. The proof of our main results is presented in Section 3.

## 2 Preliminaries

In this section, we introduce some lemmas which play a crucial role in proof of our main result in next section.

**Lemma 2.1**. *E*(*t*) is a non-increasing function.

**Lemma 2.2**. Assume that

*g*(

*t*) satisfies assumptions (A1) and (A2),

*H*(

*t*) is a twice continuously differentiable function and satisfies

for every *t* ∈ [0, *T*_{0}), and (*u*(*x*, *t*), *v*(*x*, *t*)) is the solution of the problem (1.2).

Then the function *H*(*t*) is strictly increasing on [0, *T*_{0}).

for every *t* ∈ [0, *T*_{0}).

for every *t* ∈ [0, *T*_{0}).

for every *t* ∈ [0, *T*_{0}).

Because *g*(*t*) satisfies (A2), then *h*'(*t*) ≥ 0, which implies that *h*(*t*) ≥ *h*(0) = *H*(0). Moreover, we see that *H*'(0) > *h*'(0).

*t*

_{0}> 0 and

*H*' (

*t*

_{0}) =

*h*' (

*t*

_{0}), and have

This contradicts *H*'(*t*_{0}) = *h*'(*t*_{0}). Thus, we have *H*'(*t*) > *h*' (*t*) *≥* 0, which implies our desired result. The proof of Lemma 2.2 is complete.

then
is strictly increasing on [0, *T* ).

**Proof**. Since , and (

*u*(

*t*),

*v*(

*t*)) is the local solution of problem (1.2), by a simple computation, we have

Therefore, by Lemma 2.2, the proof of Lemma 2.3 is complete.

**Lemma 2.4**. If , (

*u*

_{1},

*v*

_{1}) ∈

*L*

^{2}(Ω) ×

*L*

^{2}(Ω) satisfy the assumptions in Theorem 1.2, then the solution (

*u*(

*x*,

*t*),

*v*(

*x*,

*t*)) of problem (1.2) satisfies

for every *t* ∈ [0, *T*).

**Proof**. We will prove the lemma by a contradiction argument. First we assume that (2.9) is not true over [0,

*T*), it means that there exists a time

*t*

_{1}such that

*I*(

*u*(

*t*,

*x*),

*v*(

*t*,

*x*)) < 0 on [0,

*t*

_{1}), by Lemma 2.3 we see that is strictly increasing over [0,

*t*

_{1}), which implies

Obviously, (2.15) contradicts to (2.12). Thus, (2.9) holds for every *t* ∈ [0, *T*).

for every *t* ∈ [0, *T*). The proof of Lemma 2.4 is complete.

## 3 The proof of Theorem 1.2

where *t*_{2}, *t*_{3} and *a* are certain positive constants determined later.

which means that *G*"(*t*) > 0 for every *t* ∈ (0, *T*).

Since *G*'(0) ≥ 0 and *G*(0) ≥ 0, thus we obtain that *G*' (*t*) and *G*(*t*) are strictly increasing on [0, *T*).

which implies that *B*^{2} - *AC* ≤ 0.

*u*(

*t*,

*x*),

*v*(

*t*,

*x*)) to the problem (1.2) exists for every

*t*∈ [0,

*T*), then for

*t*∈ [0,

*T*), one has

for every *t* ∈ [0, *T*), which means that the function *G* ^{
-β
} is concave.

The proof of Theorem 1.2 is complete.

## Declarations

### Acknowledgements

This work is supported in part by NSF of PR China (11071266) and in part by Natural Science Foundation Project of CQ CSTC (2010BB9218).

## Authors’ Affiliations

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