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Titlebook: Introductory Attitude Dynamics; F. P. J. Rimrott Book 1989 Springer-Verlag New York Inc. 1989 Rotor.dynamics.moon.platform.satellites

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F. P. J. Rimrottlphabetical order.Strict alphabetical listing of all entriesVascular biology has become one of the most exciting fields in the biomedical sciences. The development of molecular biology and of genetic approaches in the mouse embryo has large­ ly contributed to our current understanding of the biology
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lphabetical order.Strict alphabetical listing of all entriesVascular biology has become one of the most exciting fields in the biomedical sciences. The development of molecular biology and of genetic approaches in the mouse embryo has large­ ly contributed to our current understanding of the biology
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The Gyroscope,utside. The quantity . is the . (or the .) of the gyroscope, and . is its first derivative with respect to time. The torque . and the angular momentum . are taken with respect to the same reference point.
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Libration,or of satellites, we shall investigate a few simple special cases. Because it exhibits strong sensitivity to the gravity gradient, among all possible satellite configurations, we select a one-dimensional rod satellite, with an inertia tensor of, say,.We assume that the satellite is very small, i.e.,
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Stability of Satellite Attitude in a Central Force Field,s used frequently by space engineers for satellites stabilized by taking advantage of the gradient of the gravitational field surrounding the master, the gradient of the field being none other than the Kepler force ., which, because of the finite size of the satellite, also exerts a torque on the sa
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Deformable Axisymmetric Gyros,oating coordinate system, the latter is used to obtain suitable equations of gyrodynamics for deformable bodies. The concept of a body of constant configuration in a floating coordinate system is introduced. The theory is then demonstrated on typical examples.
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Rigid Gyrostats,ut its axis of symmetry with respect to the platform. The rotor spin consequently does not affect the mass distribution of the gyrostat. Thus the inertia tensor of the gyrostat remains constant, provided of course that a platform and rotor are both rigid bodies.
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