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Port-Hamiltonian formulation and symplectic discretization of plate models Part Ⅰ: Mindlin model for thick plates

机译:Port-Hamiltonian公式和板模型的辛离散化Ⅰ:厚板的Mindlin模型

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The mechanical model of a thin plate with boundary control and observation is presented as a port-Hamiltonian system (PHs(1)), both in vectorial and tensorial forms: the Kirchhoff-Love model of a plate is described by using a Stokes-Dirac structure and this represents a novelty with respect to the existing literature. This formulation is carried out both in vectorial and tensorial forms. Thanks to tensorial calculus, this model is found to mimic the interconnection structure of its one-dimensional counterpart, i.e. the Euler-Bernoulli beam.The Partitioned Finite Element Method (PFEM2) is then extended to obtain a suitable, i.e. structure-preserving, weak form. The discretization procedure, performed on the vectorial formulation, leads to a finite-dimensional port-Hamiltonian system. This part II of the companion paper extends part I, dedicated to the Mindlin model for thick plates. The thin plate model comes along with additional difficulties, because of the higher order of the differential operator under consideration. (C) 2019 Elsevier Inc. All rights reserved.
机译:具有边界控制和观察功能的薄板的力学模型以矢量形式和张量形式表示为Port-Hamiltonian系统(PHs(1)):使用Stokes-Dirac描述了板的Kirchhoff-Love模型结构,这相对于现有文献而言是新颖的。该制剂以矢量和张量形式进行。借助张量演算,发现该模型可以模拟其一维对应物的互连结构,即Euler-Bernoulli梁。然后扩展了分区有限元方法(PFEM2),以获得合适的即保持结构的弱结构形成。对矢量公式执行离散化程序会导致有限维波特-汉密尔顿系统。随附纸的第二部分扩展了第一部分,该部分专门用于厚板的Mindlin模型。由于要考虑的微分算子的阶数较高,因此薄板模型会带来额外的困难。 (C)2019 Elsevier Inc.保留所有权利。

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