The Force Tracking Moment Action on the Gyrostat Motion
- 作者: Makeev N.N.
- 期: 编号 1 (64) (2024)
- 页面: 24-32
- 栏目: Mechanics
- URL: https://journal-vniispk.ru/1993-0550/article/view/307266
- DOI: https://doi.org/10.17072/1993-0550-2024-1-24-32
- ID: 307266
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The gyrostat moves around a fixed point under the forces influence in pseudo-Euclidean space with signature (3,1). The resulting moment of the external forces system and the gyrostatic moment are specified relative to the coordinate orthoreper, invariably associated with the gyrostat carrier, and are constant. Three types of gyrostat motion are given, in each of which the resulting force vector-moment is collinear to of the main axis of the gyrostat inertia, and the gyrostatic moment is orthogonal to this axis. The vector manifold of the gyrostat angular velocities and the field of its phase trajectories in the state space are found with the parametric integration method using. Integration of the gyrostat motion equations is carried out in quadratures and elliptic functions of time.
作者简介
N. Makeev
编辑信件的主要联系方式.
Email: nmakeyev@mail.ru
Doctor of Physical and Mathematical Sciences, Professor
俄罗斯联邦, Saratov, Russia参考
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- Makeev, N.N. (1979), "Ustoychivost` permanentnykh vrashcheniy girostata v prostranstve ", Differentsial`naya geometriya: mezhvuzovskiy nauchnyy sb., vol. 4, pp.150-156.
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- Smol`nikov, B.A., Stepanova, M.V. (1981), "Permanent rotations of the gyrostat with self-excitation", Izvestiya Akademii nauk. Mekhanika tvyerdogo tela, vol. 3, pp.107-113.
- Grammel, R. (1958), "Theory of asymmetric gyroscope with reactive drive", Mekhanika: period. sb. perevodov inostr. statey, vol. 6, pp. 145-151.
- Magnus, K. (1974), Giroskop. Teoriya i primenenie [Gyroscope. Theory and application], Mir, M., Russia. 528 p.
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