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Global existence of a coupled Euler-Bernoulli plate system with variable coefficients
Boundary Value Problems volume 2014, Article number: 169 (2014)
In this paper, we study the initial boundary value problem of a coupled Euler-Bernoulli plate system with spatially varying coefficients of viscosity, damping and source term in a bounded domain. We prove that under some conditions on the initial value, the growth orders of the damping terms and the source terms the solution to the problem exists globally.
MSC: 35L70, 35L75, 93D20.
The purpose of this paper is to present the global existence result of the solution to a coupled Euler-Bernoulli plate system with variable coefficients.
Let Ω be a bounded domain in with smooth boundary and . We shall consider the following initial-boundary value problem for a coupled Euler-Bernoulli plate system with variable coefficients:
in which the constants , , , and
where are functions in satisfying
λ is a positive constant. is the so-called co-normal derivative and is the unit normal of Γ pointing towards the exterior of Ω. In physical terms the entries are related to the coefficients of elasticity.
We suppose that () is the density (the mass per unit length) of the plates respectively, and it satisfies the following hypothesis:
where is a constant. We also assume that there exists a function such that
and suppose that satisfies
in which is a positive constant, for , and for .
The systems of plate equation have been studied by numerous authors, see –. Messaoudi  considered the semilinear Petrovsky equation with the damping and the source term, showed that the solution blows up in finite time if the growth order of damping term is larger than the growth order of source term and the energy is negative, whereas the solution is global if the growth order of damping term is not larger than the growth order of source term. Hoffmann and Rybka  studied the analyticity of the nonlinear term forces convergence of solutions for two equations of continuum mechanics. They showed that any solution with appropriate boundary and initial conditions has a limit as t goes to infinity. Yao  discussed the initial-boundary value problem for Euler-Bernoulli plate with variable coefficients and gave the observability inequality. The authors of  were interested in the case of thermoelastic plate and they established stability of the rest state. The authors of  discussed the exponential attractors for an extensible beam equation.  differs from ,  because  included a viscous term . This term played an important role in their consideration. Guesmia  considered the system of plate equations with damping, proved that the solution decays exponentially if the damping term behaves like a linear function, whereas the decay is of a polynomial order otherwise. Li and Wu  discussed the plate stabilization problem with infinite damping and showed that the energy of the problem decays exponentially provided that the negative damping is sufficiently small. For the Cauchy problem of multidimensional generalized double dispersion equation, Xu and Liu  proved the existence and nonexistence of global weak solution by the potential well method. Komornik and Zuazua  considered a wave equation with mixed boundary condition. They showed the stabilization without a geometrical hypothesis on the domain. This is an original work that used the multiplicative technique in the study of asymptotic behavior of a dissipative system in PDE using the energy method.
Our purpose in this paper is to give the global existence of the solution to the initial boundary value problem for a coupled Euler-Bernoulli plate system with variable coefficients.
The present work is organized as follows. In Section 2, we give the local existence result of problem (1.1). Section 3 is devoted to the global existence of the solution.
We shall write denoting the usual norm , denoting the usual norm , denoting the usual inner product in .
Let be the best constant of the embedding inequality such that
2 Local existence result
In order to state our main results, we introduce the definition of weak solution for system (1.1).
By a weak solution of system (1.1) on , we mean functions , , satisfying
for all text functions and almost all .
(Local weak solution)
Suppose the validity of assumptions (1.2)-(1.5). Then there exists a unique local weak solutionto system (1.1) defined onfor some.
Similar to .
We define the energy of system (1.1) by
Suppose the validity of assumptions (1.2)-(1.5). Then the energy function of system (1.1) satisfies the energy identity,
Multiplying the first equation of (1.1) by and the second equation of (1.1) by , integrating over and summing them, by a straightforward calculation we obtain (2.2). □
3 Global existence result
In this section, we give the global existence of system (1.1).
Suppose thatis the unique weak solution of system (1.1), the initial datasatisfy
Then the solutionis global.
From the continuity of and , we have the continuity of on .
From the assumption , it is not difficult to see that . Next we show that and is arbitrary. From the definition of and , we can rewrite for as
Thus from the nonincreasing property of (2.2), it follows that for ,
From assumptions (1.5)-(1.6) and estimate (3.3), we get that for ,
Then it follows that for small enough,
Thanks to the assumption of , we have
Thus, by selecting , we get
for . This implies . If , then it follows that for . By the uniqueness of the solution to system (1.1), we obtain that the solution is zero solution for . Then the solution is global.
For the case , from the definition of , we have and for , where is arbitrary and the following estimate holds:
Then the global existence of the solution follows. □
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The authors are highly grateful for the referees’ careful reading and comments on this paper. The research is supported by NNSFC No. 61374089 and Shanxi Scholarship Council of China No. 2013-013.
The authors declare that they have no competing interests.
The authors declare that the study was realized in collaboration with the same responsibility. All authors read and approved the final manuscript.