经典力学的广义协变形式

General covariance expression of classical mechanics

通过在一个没有引力场的局部惯性系中给出洛伦兹张量方程,再从局部惯性系转化到一般坐标系,从而得到经典力学含gμv和Γ0μv的普遍协变方程.

It s deduce the general covariance expression of classical mechanics through giving Lorentz tensor equation in a locally inertial frame without gravity first, and then transforming it to a general frame of reference.