PHAG 发表于 2025-3-25 06:59:50
http://reply.papertrans.cn/23/2272/227164/227164_21.png发现 发表于 2025-3-25 11:15:00
http://reply.papertrans.cn/23/2272/227164/227164_22.png阴郁 发表于 2025-3-25 13:22:20
http://reply.papertrans.cn/23/2272/227164/227164_23.pngforthy 发表于 2025-3-25 18:14:25
http://reply.papertrans.cn/23/2272/227164/227164_24.png怒目而视 发表于 2025-3-25 20:03:21
Blessing Mbipom,Susan Craw,Stewart MassieWe begin this chapter with the definition of the action functional as time integral over the Lagrangian ..., ... of a dynamical system:chastise 发表于 2025-3-26 00:58:03
Yichao Lu,Ruihai Dong,Barry SmythThe main purpose of this chapter is to consider the formulation of a relativistic point particle in classical electrodynamics from the viewpoint of Lagrangian mechanics. Here, the utility of Schwinger’s action principle is illustrated by employing three different kinds of action to derive the equations of motion and the associated surface terms.clarify 发表于 2025-3-26 05:06:49
D. J. H. Burden,M. Savin-Baden,R. BhaktaWe begin this chapter by deriving a few laws of nonconservation in mechanics. To this end we first consider the change of the action under rigid space translation δ.. = δε., and δ.(..) = 0. Then the noninvariant part of the action, . is given by . and thus it immediately follows for the variation of . that . orcognizant 发表于 2025-3-26 12:07:29
http://reply.papertrans.cn/23/2272/227164/227164_28.png破裂 发表于 2025-3-26 15:21:12
Hossein Ghodrati Noushahr,Samad AhmadiWe already know that canonical transformations are useful for solving mechanical problems. We now want to look for a canonical transformation that transforms the 2. coordinates (....) to 2. constant values (.., ..), e.g., to the 2. initial values (q., p.) at time . = 0. Then the problem would be solved, . = .(.., .., .), . = .(.., .., .).我不明白 发表于 2025-3-26 19:58:21
Animal Welfare Lessons from Work on Poultry,We shall first use an example to explain the concept of adiabatic invariance. Let us consider a “super ball” of mass ., which bounces back and forth between two walls (distance .) with velocity ... Let gravitation be neglected, and the collisions with the walls be elastic. If .. denotes the average force onto each wall, then we have