1) inertial potential function
惯性势函数
2) flow potential
塑性势函数
3) inertia potential energy
惯性势能
1.
This thesis introduces the notions of "inertia potential energy" and "mechanical energy" in the non-inertial system, according to the law of motion of Newton in the non-inertial reference system, deduces the relation between the mechanical energy and work, and further deduces the law of conservation of mechanical energy and its terms in the non-inertial reference system.
该文在非惯性参照系中引入“惯性势能”和“机械能”,根据非惯性系中的牛顿运动定律,推导出非惯性系中机械能与功的关系,进而导出非惯性系中机械能守恒定律及机械能守恒的条件。
4) noniertial system
惯性势
5) universal potential energy function
普适性势能函数
6) generalized inertial potential
广义惯性势
1.
Based on generalized inertial potential,this paper first gives new type of motion e-quation for nonholonomic relative motion dynamical systems,and then discusses constructing methodof in tegral in variance for these systems,finally obtains Noether s theorem and its inverse theorem.
在引入广义惯性势的基础上，首先给出了非完整相对运动动力学系统的新型运动方程，然后讨论了该系统的积分不变量的构造方法，最后得到了该系统的Ｎｏｅｔｈｅｒ定理及其逆定理。
2.
However, Largrange’s equation of the second kind of the ideal and holonomic constraint force systems is gave in this paper, beginning from generalized inertial potential to the non-inertial reference system, and Foucault’s pendulum regular of motion is solved by this analysis mechanics method.
本文从转动非惯性系出发,引入广义惯性势概念,导出非惯性系中受理想、完整约束有势力系的拉格朗日函数和第二类拉格朗日方程的广义惯性势形式。
补充资料：伦纳德-琼斯势函数
分子式：
CAS号：
性质：描述分子间相互作用势能与作用距离定量关系的函数。当势场是球形对称时，实际分子相互作用势能函数为此式即伦纳德-琼斯势函数。式中V为势能，dAB为A，B分子的核间距，ε0和D12是决定势阱深度的参数和V=0时的核间距，图示如下。上式中12次方项是排斥势，6次方项是吸引势。故又称6～12势(6～12potential)。
CAS号：
性质：描述分子间相互作用势能与作用距离定量关系的函数。当势场是球形对称时，实际分子相互作用势能函数为此式即伦纳德-琼斯势函数。式中V为势能，dAB为A，B分子的核间距，ε0和D12是决定势阱深度的参数和V=0时的核间距，图示如下。上式中12次方项是排斥势，6次方项是吸引势。故又称6～12势(6～12potential)。
说明：补充资料仅用于学习参考，请勿用于其它任何用途。
参考词条