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第三百七十三章 里奇的流形(流形)(1 / 2)

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1884年,里奇-库尔巴斯托罗(Ricci-Curbastro)开始了关于绝对微积分(absolute differential calculus)的工作。

1900年,列维-齐维塔(Levi-Civita)和里奇-库尔巴斯托罗(Ricci-Curbastro)出版了《绝对微积分方法及其应用》(Méthodes de calcul differential absolu et leures applications),其中他们建立了张量理论,15年后在广义相对论中用到。

列维-齐维塔对里奇说:“想要确认是不是拓扑学等价,也需要经过拓扑等价变化得来的。”

里奇说:“等价变换的过程,就意味着这个东西需要做一个改变了,尤其是曲率会有改变。”

列维说:“听起来好复杂啊,能够完成吗?”

里奇说:“会的,复杂但不意味着做不到,一个有曲率的流形,可以用埃尔米特度量来表示,曲率的变换,仅仅是那些上三角矩阵中数字的变换而已。”

列维说:“我们可以尝试的去掌握这种变换。”

里奇想拿热学做类比,但是实际不成熟,脑中想了想之后,还是压下去低调的说:“没错,到时候等价拓扑流形变换,就是埃尔米特流形度量矩阵里数字的变化而已。那个时候,我们可以使用这个工具去构造。”里奇突然在想,很多热力学中的复杂变化跟这个里奇流变化也有关系,而且埃尔米特度量矩阵中的数字,有了一种类似于玻尔兹曼公式中的热学信息的秩序感,那么热学中的无序变化,就是热学中埃尔米特度量的数字信息的变化,从这个数字上可以反映出有序到无序的不可逆性,就类似了棋盘和摆牌这种模型了。

列维说:“然后用它可以完成一系列的拓扑手术,构造几何结构,把不规则的流形变成规则的流形。这个可以应用在力学中,力学可以让材料发生变形。力学几何解释就是,内在的曲率变化就是封闭流形的度规变化的原因。把局部内在转动归结为封闭流形位形几何演化的内在原因。”

里奇觉得力学的比喻是十分恰当的,而且还找到了变化的单元,借助这个局部转动的概念,就可以像垒积木一样的搭建一个流形大厦了。

同时他认为可以从两个角度来解释:“对连续介质力学而言,对dg/dt 可以作出应变的对应解释。而在几何上,对于曲率变化,可以做出局部内在转动的解释。”

列维说:“所以,把局部内在转动归结为封闭流形位形几何演化的内在原因。如果这个内在转动不为零,则封闭流形会演化下去,只到达成一个平衡位形。”

一般而言,外部的物理作用由一个泛函f引入,从而,完整的、在外场作用下的Ricci方程为:

dg/dt=-2Ricci(g)-2ddf(R)。

这样,对特定的外场,就有一个特定的平衡位形。

与连续介质力学不同,应力的概念被一个依赖于曲率的泛函局部二阶微分特性给定了。

这多少与格林应力是等价的。

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