Titlebook: Rotational Dynamics of Orbiting Gyrostats; Department of Genera Robert E. Roberson,Pierre Y. Willems,Jens Wittenbu Book 1971 Springer-Verla

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Robert E. Roberson,Pierre Y. Willems,Jens Wittenburg

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Axial Gyrostats, Canonical Cases, axial gyrostat for which h. = h. = 0 , h. > 0. It is convenient to dispose first of the special body shapes, as in the case of the osculation study. For the Sphere, the axial case is the only case, so the solution given for it completely disposes of that body shape.

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Axial Gyrostats, Canonical Cases,o the development of analytical solutions for the angular velocity components. In the present section, we confine ourselves to the special case of the axial gyrostat for which h. = h. = 0 , h. > 0. It is convenient to dispose first of the special body shapes, as in the case of the osculation study.

Impugn

The General Free Gyrostat : Recent Investigations,on have been discussed. In the following we will consider the torque-free motion of the unsymmetrical gyrostat with a rotor which is not aligned with a principal axis nor does it lie in the plane of two principal axes. Since the polhodes, i.e. the intersection lines of the energy and the angular mom

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The General Free Gyrostat (continued),rical gyrostat with three non-zero components h. of relative angular rotor momentum is considered. Then, two integrals of motion are available: . Hence, of the three differential equations of motion only one is needed to determine together with (1) and (2) ω. as functions of time. We select the thir