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首页> 外文期刊>Journal of Differential Equations >A unified approach via convexity for optimal energy decay rates of finite and infinite dimensional vibrating damped systems with applications to semi-discretized vibrating damped systems
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A unified approach via convexity for optimal energy decay rates of finite and infinite dimensional vibrating damped systems with applications to semi-discretized vibrating damped systems

机译:有限元和无限维减振系统通过凸度实现最佳能量衰减率的统一方法,并应用于半离散减振系统

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The Liapunov method is celebrated for its strength to establish strong decay of solutions of damped equations. Extensions to infinite dimensional settings have been studied by several authors (see e.g. Haraux, 1991 [11], and Komornik and Zuazua, 1990 [17] and references therein). Results on optimal energy decay rates under general conditions of the feedback is far from being complete. The purpose of this paper is to show that general dissipative vibrating systems have structural properties due to dissipation. We present a general approach based on convexity arguments to establish sharp optimal or quasi-optimal upper energy decay rates for these systems, and on comparison principles based on the dissipation property, and interpolation inequalities (in the infinite dimensional case) for lower bounds of the energy. We stress the fact that this method works for finite as well as infinite dimensional vibrating systems and as well as for applications to semi-discretized nonlinear damped vibrating PDE's. A part of this approach has been introduced in Alabau-Boussouira (2004, 2005) [1,2]. In the present paper, we identify a new, simple and explicit criteria to select a class of nonlinear feedbacks, for which we prove a simplified explicit energy decay formula comparatively to the more general but also more complex formula we give in Alabau-Boussouira (2004, 2005) [1,2]. Moreover, we prove optimality of the decay rates for this class, in the finite dimensional case. This class includes a wide range of feedbacks, ranging from very weak nonlinear dissipation (exponentially decaying in a neighborhood of zero), to polynomial, or polynomial-logarithmic decaying feedbacks at the origin. In the infinite dimensional case, we establish a comparison principle on the energy of sufficiently smooth solutions through the dissipation relation. This principle relies on suitable interpolation inequalities. It allows us to give lower bounds for the energy of smooth initial data for the one-dimensional wave equation with a distributed polynomial damping, which improves Haraux (1995) [12] lower estimate of the energy for this case. We also establish lower bounds in the multi-dimensional case for sufficiently smooth solutions when such solutions exist. We further mention applications of these various results to several classes of PDE's, namely: the locally and boundary damped multi-dimensional wave equation, the locally damped plate equation and the globally damped coupled Timoshenko beams system but it applies to several other examples. Furthermore, we show that these optimal energy decay results apply to finite dimensional systems obtained from spatial discretization of infinite dimensional damped systems. We illustrate these results on the one-dimensional locally damped wave and plate equations discretized by finite differences and give the optimal energy decay rates for these two examples. These optimal rates are not uniform with respect to the discretization parameter. We also discuss and explain why optimality results have to be stated differently for feedbacks close to linear behavior at the origin.
机译:Liapunov方法因其建立阻尼方程解的强衰减性而闻名。数位作者已经研究了对无穷维设置的扩展(参见例如Haraux,1991 [11],以及Komornik和Zuazua,1990 [17]以及其中的参考文献)。在反馈的一般条件下,最佳能量衰减率的结果还远远不够完整。本文的目的是表明一般的耗散振动系统具有由于耗散而产生的结构特性。我们提出了一种基于凸度参数的通用方法,可为这些系统建立尖锐的最佳或准最佳上限能量衰减率,并基于耗散特性和插值不等式(在无穷维情况下)的比较原理来确定下限。能源。我们强调了这样一个事实,即该方法适用于有限维和无限维振动系统,以及适用于半离散非线性阻尼PDE振动的应用。这种方法的一部分已在Alabau-Boussouira(2004,2005)[1,2]中引入。在本文中,我们确定了一个新的,简单且显式的准则来选择一类非线性反馈,为此,我们证明了一种简化的显式能量衰减公式,与我们在Alabau-Boussouira(2004)中给出的更一般但更复杂的公式相比,2005)[1,2]。此外,我们证明了在有限维情况下此类衰减率的最优性。此类包括范围广泛的反馈,从非常弱的非线性耗散(在零附近​​呈指数衰减)到原点的多项式或多项对数衰减反馈。在无穷维情况下,我们通过耗散关系对足够光滑的解的能量建立了比较原理。该原理依赖于合适的插值不等式。它使我们能够为具有分布多项式阻尼的一维波动方程的平滑初始数据提供能量的下界,从而改善了Haraux(1995)[12]在这种情况下对能量的较低估计。当多维解中存在足够平滑的解时,我们还会为其设置下界。我们进一步提到将这些各种结果应用到几类PDE中,即:局部和边界阻尼多维波动方程,局部阻尼板方程和整体阻尼耦合Timoshenko梁系统,但它也适用于其他几个示例。此外,我们表明,这些最佳能量衰减结果适用于从无限维阻尼系统的空间离散化获得的有限维系统。我们用有限差分离散的一维局部阻尼波和板方程来说明这些结果,并给出这两个示例的最佳能量衰减率。这些最佳速率相对于离散化参数而言是不一致的。我们还将讨论和解释为什么对于接近于原点线性行为的反馈,最优结果必须以不同的方式陈述。

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