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第三百七十三章 里奇的流形(流形)(2 / 2)

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而在连续介质力学中,一个长期以来的难题是如何定义物质微元的几何属性。

这个物质微元是封闭的3-流形。

从而,Ricci流方程把微元闭流形的变化与连续介质的宏观位形变化连续了起来。

而在经典的连续介质力学中,微元物质是被隐涵的假定为三个1-流形的直和。

那是最为简单的情况,这是特例。此时,各向同性假定是必须引入的。

但是,各向异性就象一个幽灵,紧随大变形而来,如接受,就与前提矛盾;如不接受,又与客观事实矛盾。因而,理性力学一直在这个问题上纠结不清。

在上世纪50年代后,一个流形的概念是把物质微元看成是一个2-流形与一个1-流形的直和。这就是所谓的:有极介质。它的最终成果就是液晶。

一个更为普遍性的介质是:具有某种旋转对称性的各向异性介质。(旋转对称轴是1-流形,旋转曲面是2-流形。)

对任意的微元为3-流形的介质,唯一的办法是引入先天性的3个独立矢(或者是任意的3-流形g(0)。)而这就是Ricci流。

这样的一种描述才是现代材料科学所需求的连续介质力学的最基本的理论体系。

我国力学家陈至达建立的理性力学理论体系事实上就是按引入先天性的3个独立矢来构造的。

但是,只完成了几何部分,没有建立相应的外场介入形式,而Ricci流方程恰恰是一个最为有力的补充。这样,一个更为深刻的理论构造方向就大门洞开了。

事实上,Truesdell, Noll,等等的后期理性力学一致的指向:连续介质力学的微元物质概念。

我们能够看到的是:Ricci流概念建立于上世纪80年代,在几何上并没有超前于理性力学。但是,在物理原因的描述上的确是超前于理性力学。

换句话说:Ricci流概念为理性力学与现代物理的结合打开了一扇大门,而陈理性力学是与Ricci流概念协调的变形力学体系。我走在了正确的道路上。这是值得自豪的。

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