Introduction T simulation of attitude motions of highly deformable, dissipative spacecraft is so difficult that one is highly motivated to resort to heuristic methods of analysis, particularly when the deformability and/or dissipation characteristics of the spacecraft are not well defined, as during preliminary design. One such method is the so-called energy-sink approach, which has been used extensively' to obtain qualitative and quantitative information regarding attitude motions of relatively simple spacecraft. However, the use of this technique is frequently accompanied by rather strong disclaimers,'''' which suggests that the designer is well-advised to view it with suspicion. More particularly, when the spacecraft under consideration contains driven rotors, as when momentum wheels or control moment gyros are employed for attitude control, one must entertain doubts regarding the validity of energy-sink arguments, for such components of a spacecraft can play the roles of energy sources, a fact first pointed out by Landon and Stewart. Nevertheless, the method has been employed even under these circumstances; and, although some published work contains material showing that incorrect conclusions can be reached in this way, failure of the energy-sink approach has not been the central issue in anything that has appeared in print to date, with the result that the dangers inherent in the use of the method remain obscure. The present paper is intended to remedy this situation. This paper begins with the development of a formula that enables one to find the angle (nutation angle) between the central angular momentum vector and the symmetry axis of a torque-free, axisymmetric gyrostat as a function of the system's kinetic energy of rotation. A suitable kinetic energy time-history reflecting energy dissipation is then postulated, and the formula is used to construct a plot of the nutation angle as a function of time. To compare this energy-sink prediction with the actual motion of a deformable spacecraft, a gyrostat carrying a nutation damper is. considered next. This system has deformability and energy dissipation capabilities of the kind one must deal with when analyzing large, flexible spacecraft, but it is sufficiently simple to permit the formulation of exact differential equations of motion.
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