An orbital tether system, including a satellite (a rigid body), an elastic ponderable tether and a terminal load, is investigated. A mathematical model is obtained using Lagrange's equation of the second kind, which enables the plane translational motion of the centres of mass of the elements of the
The oscillations of a body with an orbital tethered system
β Scribed by V.S. Aslanov
- Publisher
- Elsevier Science
- Year
- 2007
- Tongue
- English
- Weight
- 199 KB
- Volume
- 71
- Category
- Article
- ISSN
- 0021-8928
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β¦ Synopsis
The motion about a centre of mass of a rigid body with a tethered system, designed to launch a re-entry capsule from a circular orbit is considered. In the deployment of the tethered system the direction and value of the tensile strength of the tether vary and, if the point of application of the tensile strength does not coincide with the centre of mass of the body, a moment occurs which leads to oscillations of the body with variable amplitude and frequency. A non-linear equation of the perturbed motion of the body about the centre of mass under the action of the tensile force of the tether and the gravitational moment is derived. Assuming that the change in the value and direction of the tensile force is slow and also that the gravitational moment is small, approximate and exact solutions of the non-linear differential equation of the unperturbed motion are obtained in terms of elementary functions and elliptic Jacobi functions. For perturbed motion, the action integral is expressed in terms of complete elliptic integrals of the first and second kind.
π SIMILAR VOLUMES
The problem of the motion of an orbital pendulum suspended on a tether is considered. The existence of relative equilibria is investigated, as well as the sufficient conditions for their stability. Particular attention is paid to the study of coupling reactions, in particular, the question of whethe
It is established that oscillations in the low-frequency range are characteristic for a body with a heavyrigid spike-shaped inclusion, and corresponding modes mainly occur as flexural deformations of the tip of the spike, localized close to its vertex.