复合材料热波过程的最优控制

Aleksei P. Zhabko, Vladimir V. Karelin, Vyacheslav V. Provotorov, Sergey M. Sergeev
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引用次数: 0

摘要

本文提出了用于分析复合材料(复合材料)结构元件热波过程最优控制问题的惩罚函数方法及其相应的惩罚函数方法。考虑了一种在工业领域中非常常见的对象,其结构是一组单向复合材料的层(相)-层状复合材料。在解决与复合材料状态的分析和描述有关的问题时,为了不解决非均匀介质的相应问题,通常使用不是介质各点坐标函数的层的定量特性。这样的函数是Sobolev空间的元素,首先是可与平方求和的函数。其便利性在于,在寻找各种类型的初边值问题(在大多数情况下,这类问题是许多物理过程的数学模型的基础)的可解性条件时,可以将其简化为算子差分系统,因此很容易构造弱解的先验估计。在建立了复合材料热或波过程的初边值问题的弱可解性之后,下一步就是这些过程的最优控制问题的表述和求解。文中提出的罚函数法是解决这类问题的一般方法。它不仅适用于标量函数的椭圆型、抛物型等问题(包括非线性问题),也适用于向量函数。后者的一个例子是Navier-Stokes系统,广泛用于描述类网络流体动力过程,考虑在Sobolev空间中,其元素是n维类网络域上的带有载波的函数,n大于或等于2。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Optimal control of thermal and wave processes in composite materials
The paper indicates the approach and the corresponding to it method of penalty functions for analyzing the problems of optimal control of thermal and wave processes in structural elements made of composite materials (composites). An object that is quite common in the industrial sphere, the structure of which is a set of layers (phases) of unidirectional composites — layered composites, is considered. When solving problems related to the analysis and description of the states of composites, quantitative characteristics of layers that are not functions of the coordinates of the points of the medium are usually used in order not to solve the corresponding problems for an inhomogeneous medium. Such functions are elements of Sobolev spaces, first of all, functions summable with a square. The convenience lies in the fact that when finding the conditions for solvability of initial-boundary value problems of various types (in most cases, such problems are the basis of mathematical models of many physical processes), it is possible to reduce to operator-difference systems, for which it is easy to construct a priori estimates of weak solutions. The next step after establishing the weak solvability of the initial-boundary value problem of the thermal or wave process in composites is the formulation and solution of the problem of optimal control of these processes. The proposed method of penalty functions on the example of solving such problems is a general method. It is applicable with slight modifications also not only in the case of elliptic, parabolic and other problems (including nonlinear) for scalar functions, but also for vector functions. An example of the latter is the Navier–Stokes system, widely used in the description of network-like hydrodynamic processes, considered in Sobolev spaces, the elements of which are functions with carriers on n-dimensional network-like domains, n greater or equal to 2.
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