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动量矩变量描述的陀螺体永久转动的分岔特性 总被引:2,自引:0,他引:2
本文建立以动量矩分量和Deprit正则变量为独立变量的陀螺体动力学方程,用以描述无力矩非对称陀螺体的姿态运动。在动量矩空间内讨论了陀螺体永久转动轴的数目和稳定性随转子转速变化的分岔特性。 相似文献
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基于Rodrigues参数的陀螺体受控运动 总被引:1,自引:0,他引:1
经典刚体动力学中表示刚体姿态的参数中,Euler角、Cardan角和Euler参数在工程技术中使用最为普遍.近期在航天器姿态控制问题中使用Rodrigues参数的报道也引起注意,Rodrigues参数以其表达形式简明和代数运算特点而具有独特优点.航天器姿态控制系统必须具有自适应性以适应参数的变化,建立用Rodrigues参数表达的无力矩陀螺体受控运动方程,提出基于Rodrigues参数的自适应姿态控制方案,并应用Lyapunov定理证明受控运动的渐近稳定性。 相似文献
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A master–slave scheme for global robust synchronization of two electro-mechanical gyrostat systems with time-varying phase mismatches under variable substitution control is presented in this paper. Under this scheme, a sufficient criterion for the global robust synchronization with bounded error is rigorously proved in the form of matrix inequality and the corresponding estimated error bound is mathematically given. On the basis of the criterion, further derivation brings some simple and optimized algebraic criteria for various single-variable coupling, whose performance is then verified through some numerical examples. 相似文献
5.
Mohammad Pourmahmood Aghababa Hasan Pourmahmood Aghababa 《Mechanics Research Communications》2011,38(7):500-505
This paper deals with the problem of robust finite-time stabilization of non-autonomous chaotic gyrostat systems. It is assumed that the parameters of the gyrostat system are completely unknown in advance and the system is perturbed by unknown uncertainties and disturbances. Some update laws are proposed to estimate the unknown parameters. Based on the finite-time control idea and the update laws, appropriate control laws are designed to ensure the stabilization of the closed-loop system in a finite time. The finite-time stability and convergence of the closed-loop system are analytically proved. A numerical simulation is given to demonstrate the applicability and robustness of the proposed finite-time controller and to verify the theoretical results. 相似文献
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María del Carmen Balsas Elena S. Jiménez Juan A. Vera Antonio Vigueras 《Central European Journal of Physics》2009,7(1):67-78
In this paper, we consider an integrable approximation of the planar motion of a gyrostat in Newtonian interaction with a
spherical rigid body. We then describe the Hamiltonian dynamics, in the fibers of constant total angular momentum vector of
an invariant manifold of motion. Finally, using the Liouville-Arnold theorem and a particular analysis of the momentum map
in its critical points, we obtain a complete topological classification of the different invariant sets of the phase flow
of this problem. The results can be applied to study two-body roto-translatory problems where the rotation of one of them
has a strong influence on the orbital motion of the system.
相似文献
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Dan Comănescu 《Mathematical Methods in the Applied Sciences》2013,36(4):373-382
We study the stability of the equilibrium points of a skew product system and analyze the possibility to construct a Lyapunov function by using a set of conserved quantities and solving an algebraic system. We apply the theoretical results to study the stability of an equilibrium state of a heavy gyrostat in the Zhukovski case. Copyright © 2012 John Wiley & Sons, Ltd. 相似文献
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Juan Antonio Vera López 《Central European Journal of Physics》2009,7(4):677-689
In this paper we consider the noncanonical Hamiltonian dynamics of a gyrostat in the three-body problem. By means of geometric
mechanics methods, we study the approximate Poisson dynamics that arise when we develop the potential of the system in Legendre
series and truncate this to an arbitrary order k. After reduction of the dynamics by means of the two symmetries of the system, we consider the existence and number of equilibria
which we denominate of Lagrangian type, in analogy with classic results on the topic. Necessary and sufficient conditions
are established for their existence in an approximate dynamics of order k, and explicit expressions for these equilibria are given, this being useful for the subsequent study of their stability.
The number of Lagrangian equilibria is thoroughly studied in approximate dynamics of orders zero and one. The main result
of this work indicates that the number of Lagrangian equilibria in an approximate dynamics of order k for k ≥1 is independent of the order of truncation of the potential, if the gyrostat S
0 is almost spherical. In relation to the stability of these equilibria, necessary and sufficient conditions are given for
linear stability of Lagrangian equilibria when the gyrostat is almost spherical. In this way, we generalize the classical
results on equilibria of the three-body problem and many results provided by other authors using more classical techniques
for the case of rigid bodies.
相似文献
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