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Free motion equation : ウィキペディア英語版
Free motion equation
A free motion equation is a differential equation that describes a mechanical system in the absence of external forces, but in the presence only of an inertial force depending on the choice of a reference frame.
In non-autonomous mechanics on a configuration space Q\to \mathbb R, a free motion equation is defined as a second order non-autonomous dynamic equation on Q\to \mathbb R which is brought into the form
: \overline q^i_=0
with respect to some reference frame (t,\overline q^i) on Q\to \mathbb R. Given an arbitrary reference frame (t,q^i) on Q\to \mathbb R, a free motion equation reads
: q^i_=d_t\Gamma^i +\partial_j\Gamma^i(q^j_t-\Gamma^j) -
\frac\frac(q^j_t-\Gamma^j) (q^k_t-\Gamma^k),
where \Gamma^i=\partial_t q^i(t,\overline q^j) is a connection on Q\to \mathbb R associates with the initial reference frame (t,\overline q^i). The right-hand side of this equation is treated as an inertial force.
A free motion equation need not exist in general. It can be defined if and only if a configuration bundle
Q\to\mathbb R of a mechanical system is a toroidal cylinder T^m\times \mathbb R^k.
== References ==

* De Leon, M., Rodrigues, P., Methods of Differential Geometry in Analytical Mechanics (North Holland, 1989).
* Giachetta, G., Mangiarotti, L., Sardanashvily, G., Geometric Formulation of Classical and Quantum Mechanics (World Scientific, 2010) ISBN 981-4313-72-6 ((arXiv: 0911.0411 )).

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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