设计高效的计算机实验-超越有限元建模的一步

N. Vollert, J. Schicker, C. Hirschl, Martin Kraft, J. Pilz
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引用次数: 6

摘要

现代多物理场模拟(如FEM)面临的一个共同挑战是,潜在问题变得越复杂,模拟就越依赖于一系列无法理解或难以理解的参数。同时,有限元计算时间随着问题复杂性的增加而增加,使得有限元模拟无法探索整个参数空间。从可管理数量的运行中获得尽可能多的信息显然需要涉及某种形式的实验设计(DOE),称为模拟研究的计算机实验设计(DOCE)。除了决定应该对哪些参数集进行模拟之外,这些模拟的结果还用作构建统计“元模型”的数据。通过允许从任意参数集计算任何感兴趣的变量,而无需运行新的模拟,这些元模型有助于以最佳努力有效地探索整个参数空间。因此,DOCE方法确实能够扩展和优化仅通过模拟研究就可以实现的可能性。为了在一个相对简单的例子上演示该方法,本工作的重点是设计和验证用于计算矩形单晶(100)样品中的线性单向应力的元模型。结果表明,在不同应力状态下,有限元模型与元模型的差异始终小于≈4 MPa,最大应力为215 MPa。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Designing efficient computer experiments - The step beyond finite element modelling
A common challenge in modern multi-physics simulations like FEM is that the more complex the underlying problems become, the more the simulation depends on a range of not or just poorly understood parameters. At the same time, the increase of FEM computing time with the complexity of the underlying problem makes it impossible to explore the whole parameter space with FE simulations. Gaining as much information as possible from a manageable number of runs clearly requires involving some form of Design of Experiments (DOE), referred to as Design of Computer Experiments (DOCE) for simulation studies. In addition to the decision for which parameter sets simulations should be performed, the results of these simulations are used as data for constructing a statistical “metamodel”. By enabling the calculation of any variable of interest from arbitrary parameter sets without having to run new simulations, these metamodels facilitate an efficient exploration of the entire parameter space with optimal effort. Hence, the DOCE approach is indeed capable of expanding and optimizing the possibilities already achievable by simulation studies alone. For demonstrating the method on a relatively simple example, this work is focused on designing and validating a metamodel for calculating linear, one-directional stresses in rectangular monocrystalline (100) samples. It will be shown that the differences between FEM and the metamodel are always smaller than ≈ 4 MPa for different stress states up to a maximum stress of 215 MPa.
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