Discrete physics using metrized chains

A. DiCarlo, F. Milicchio, A. Paoluzzi, V. Shapiro
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引用次数: 17

Abstract

Over the last fifty years, there have been numerous efforts to develop comprehensive discrete formulations of geometry and physics from first principles: from Whitney's geometric integration theory [33] to Harrison's theory of chainlets [16], including Regge calculus in general relativity [26, 34], Tonti's work on the mathematical structure of physical theories [30] and their discrete formulation [31], plus multifarious researches into so-called mimetic discretization methods [28], discrete exterior calculus [11, 12], and discrete differential geometry [2, 10]. All these approaches strive to tell apart the different mathematical structures---topological, differentiable, metrical---underpinning a physical theory, in order to make the relationships between them more transparent. While each component is reasonably well understood, computationally effective connections between them are not yet well established, leading to difficulties in combining and progressively refining geometric models and physics-based simulations. This paper proposes such a connection by introducing the concept of metrized chains, meant to establish a discrete metric structure on top of a discrete measure-theoretic structure embodied in the underlying notion of measured (real-valued) chains. These, in turn, are defined on a cell complex, a finite approximation to a manifold which abstracts only its topological properties. The algebraic-topological approach to circuit design and network analysis first proposed by Branin [7] was later extensively applied by Tonti to the study of the mathematical structure of physical theories [30]. (Co-)chains subsequently entered the field of physical modeling [4, 18, 24, 25, 31, 37], and were related to commonly-used discretization methods such as finite elements, finite differences, and finite volumes [1, 8, 21, 22]. Our modus operandi is characterized by the pivotal role we accord to the construction of a physically based inner product between chains. This leads us to criticize the emphasis placed on the choice of an appropriate dual mesh: in our opinion, the "good" dual mesh is but a red herring, in general.
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使用度量链的离散物理
在过去的五十年里,有许多努力从第一原理发展几何和物理的综合离散公式:从Whitney的几何积分理论[33]到Harrison的链链理论[16],包括广义相对论中的Regge微积分[26,34],Tonti对物理理论的数学结构[30]及其离散公式的研究[31],以及对所谓的模拟离散化方法[28]、离散外微积分[11,12]、离散微分几何[2,10]的各种研究。所有这些方法都力求区分支撑物理理论的不同数学结构——拓扑结构、可微结构、格律结构,以便使它们之间的关系更加透明。虽然每个组件都被很好地理解,但它们之间的计算有效联系尚未很好地建立,这导致在组合和逐步完善几何模型和基于物理的模拟方面存在困难。本文通过引入度量链的概念提出了这样一种联系,即在隐含在度量链(实值链)概念中的离散测度论结构之上建立一个离散度量结构。这些,反过来,是定义在一个细胞复合体,一个有限的近似流形,抽象其拓扑性质。首先由Branin[7]提出的电路设计和网络分析的代数-拓扑方法后来被Tonti广泛应用于物理理论的数学结构研究[30]。(Co-)链随后进入物理建模领域[4,18,24,25,31,37],与常用的有限元、有限差分、有限体积等离散化方法有关[1,8,21,22]。我们的工作方式的特点是,我们同意在链之间建立一个基于物理的内部产品的关键作用。这导致我们批评强调选择合适的双网格:在我们看来,一般来说,“好的”双网格只是转移注意力。
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