Precession motions of a gyrostat, having a fixed point, in three homogeneous force fields

The subject of investigation is the problem on precession motions of a gyrostat with a fixed point in three homogeneous force fields. The class of precessions under consideration is characterized by the constancy of the precession angle and by the commensurability of the precession and proper rotation velocities. Equations of a gyrostat motion are reduced to a system of three second order differential equations with respect to velocities of precession and proper rotation. Integration of these equations was conducted in the case of precessionally isoconic motions (the precession velocity equals to the proper rotation velocity) and in the case of 2:1 resonance, when the precession velocity is two times more, than the proper rotation velocity. It was proved that the obtained solutions can be described by elementary functions of time.

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Journal
Известия Академии наук. Российская академия наук. Механика твердого тела.
Published
2024-11-12
DOI
https://doi.org/10.31857/s1026351924020148
Primary Topic
Aerospace Engineering and Control Systems
Type
article
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article

Precession motions of a gyrostat, having a fixed point, in three homogeneous force fields

Г. В. Горр
Известия Академии наук. Российская академия наук. Механика твердого тела.
Aerospace Engineering and Control Systems
article

Precession motions of a gyrostat, having a fixed point, in three homogeneous force fields

Г. В. Горр
article en

Abstract

The subject of investigation is the problem on precession motions of a gyrostat with a fixed point in three homogeneous force fields. The class of precessions under consideration is characterized by the constancy of the precession angle and by the commensurability of the precession and proper rotation velocities. Equations of a gyrostat motion are reduced to a system of three second order differential equations with respect to velocities of precession and proper rotation. Integration of these equations was conducted in the case of precessionally isoconic motions (the precession velocity equals to the proper rotation velocity) and in the case of 2:1 resonance, when the precession velocity is two times more, than the proper rotation velocity. It was proved that the obtained solutions can be described by elementary functions of time.

Известия Академии наук. Российская академия наук. Механика твердого тела.(2)
Steklov Mathematical Institute (RU)
Openalex Percentile: Top 68%
Aerospace Engineering and Control Systems
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