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Lagrangian Dynamics

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Classical Mechanics with Mathematica®

Abstract

In this chapter, Lagrangian dynamics is described. After introducing the configuration space for a system of constrained rigid bodies, the principle of virtual power and its equivalence to Lagrange’s equations is shown. Then, these equations are formulated in the case of conservative forces and forces deriving from a generalized potential energy. The fundamental relation between conservation laws (first integrals) and the symmetries of the Lagrangian function is proved (Noether’s theorem). Further, Lagrange’s equations for linear nonholonomic constraints are formulated. The chapter contains also the analysis of small oscillations about a stable equilibrium configuration (normal modes) , and an introduction to variational calculus including Hamilton’s principle. Finally, two geometric formulations of Lagrangian’s dynamics are presented together with Legendre’s transformation that allows to transform Lagrange’s equations into Hamilton’s equations.

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Notes

  1. 1.

    More precisely, \({V}_{6{N}}\) is an open 6N-dimensional submanifold of \(\mathfrak {R}^{3{N}}\) \(\times O(3)^N\) since we must exclude those values of \({x}_{{G}_{i}1}\), \({x}_{{G}_{i}2}\), \({x}_{{G}_{i}3}\), and \(\psi _{{i}}\), \(\varphi _{{i}}\), \(\theta _{{i}}\), \(i = 1,\ldots , N\), for which parts of two or more bodies of S occupy the same region of the three-dimensional space.

  2. 2.

    In some textbooks, (17.29) is given as a definition of smooth constraints.

  3. 3.

    A wider introduction to variational calculus can be found in Chapter 27.

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Correspondence to Antonio Romano .

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Romano, A., Marasco, A. (2018). Lagrangian Dynamics. In: Classical Mechanics with Mathematica®. Modeling and Simulation in Science, Engineering and Technology. Birkhäuser, Cham. https://doi.org/10.1007/978-3-319-77595-1_17

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