Abstract
It is a well-known fact that a second order differential equation \(\ddot{x}(t)=\bar{\alpha}(t,x(t),\dot{x}(t))\) expressing Newton’s law in ℝn may be represented as a first order system on the space of dimension 2n:
We call the first equation of the above system horizontal and the second one vertical. This is consistent with the terminology in the general case of a mechanical system on a non-linear configuration space M, where Newton’s law is presented by means of covariant derivatives in the form (11.2), equivalent to equation (11.3) with a special vector field (second order differential equation) on the phase space TM. Recall that the field (11.3) is the sum of the Levi-Civitá geodesic spray \(\mathcal{Z}\) (which is horizontal, i.e. belongs to the connection) and the vertical lift of the vector force field (which belongs to the vertical subspace).
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© 2011 Springer-Verlag London Limited
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Gliklikh, Y.E. (2011). Mechanical Systems with Random Perturbations. In: Global and Stochastic Analysis with Applications to Mathematical Physics. Theoretical and Mathematical Physics. Springer, London. https://doi.org/10.1007/978-0-85729-163-9_14
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DOI: https://doi.org/10.1007/978-0-85729-163-9_14
Publisher Name: Springer, London
Print ISBN: 978-0-85729-162-2
Online ISBN: 978-0-85729-163-9
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