一般完整系统中的哈密顿正则方程

Hamiltons Canonilal equation in the General Complete System

本文在一般完整的力学系统中引入广义正则动能函数，该函数以广义坐标、广义动量和时间ｔ为变量，并且仅与系统的动能有关。在此基础上，建立了一组与一般完整系统的拉格朗日方程、哈密顿原理相对应的哈密顿正则方程。

This essay introduces the canonical momentum function in its broad sense on the basis of the enderal Mecharies system This function takes generalized coordinates, generalized momentum and time t as its variablity which makes it have dose cose connection only with the momenfum in its system this, in this way, it produces such a serics of canonical equations as Lagrange's equation, Hamilton's principle and Hamiltoon's canonical equation which is correspodert with the general system.