Resolving Absorbed Work and Generalized Inertia Forces from System Energy Equation - A Hamiltonian and Phase-Space Kinematics Approach

Tuhin Das
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Abstract

This paper develops a theoretical basis and a systematic process for resolving all inertia forces along generalized coordinates from the overall energy equation of a dynamical system. The theory is developed for natural systems with scleronomic constraints, where the potential energy is independent of generalized velocities. The process involves expansion of the energy equation, and specifically a special expansion of the kinetic energy term, from which the inertia forces emerge. The expansion uses fundamental kinematic identities of the phase space. It is also guided by insights drawn from the structure of the Hamiltonian function. The resulting equation has the structure of the D'Alembert's equation but involving generalized coordinates, from which the Lagrange's equations of motion are obtained. The expansion process elucidates how certain inertia forces manifest in the energy equation as composite terms that must be accurately resolved along different generalized coordinates. The process uses only the system energy equation, and neither the Hamiltonian nor the Lagrangian function are required. Extension of this theory to non-autonomous and nonholonomic systems is an area of future research.
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从系统能量方程中解析吸收功和广义惯性力--哈密顿和相空间运动学方法
本文建立了一个理论基础和系统过程,用于从动力学系统的总能量方程中解决沿广义坐标的所有惯性力。该理论是针对具有硬约束的自然系统开发的,其中势能与广义速度无关。这一过程涉及能量方程的展开,特别是动能项的特殊展开,惯性力就是从动能项中产生的。扩展使用了相空间的基本运动学特性。它还以从汉密尔顿函数结构中获得的启示为指导。由此得到的方程具有达朗贝尔方程的结构,但涉及广义坐标,由此得到拉格朗日运动方程。扩展过程阐明了某些惯性力如何在能量方程中表现为必须沿不同广义坐标精确解析的复合项。该过程只使用系统能量方程,不需要哈密顿和拉格朗日函数。将这一理论扩展到非自治和非全局系统是未来研究的一个领域。
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