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GP-B Post-Flight Analysis—Final Report - Gravity Probe B - Stanford ...

GP-B Post-Flight Analysis—Final Report - Gravity Probe B - Stanford ...

GP-B Post-Flight Analysis—Final Report - Gravity Probe B - Stanford ...

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9.2 Suspension Controller DesignThis section describes the design and operation of the gyro suspension controller.9.2.1 Controller description and space of operationThe position of each gyroscope rotor in its housing is sensed through and electrostatic centering forces areapplied via six circular electrodes located on the gyroscope housing wall (Figure 9-7). This non-contactsuspension eliminates gimbal and bearing torques evident in other mechanical gyroscopes. The residualelectrostatic torques that do remain are proportional to 1) the rotor’s spherical asymmetry, 2) the rotor’s massimbalance,3) spin axis misalignment from the vehicle roll axis, and 4) the magnitudes of the electrostaticsuspension fields. The GSS is designed to minimize the electrostatic suspension fields while keeping the rotorcentered against external disturbances.Figure 9-7. Photograph of rotor and housing. Suspension electrodes and spin-up channel are clearly seen.Low-torque operation requires the control authority (bandwidth) of the controller to be minimized. Thedisturbance environment, however, is characterized by random micrometeoroid strikes that can applyimpulsive disturbances as large as 10,000 times the nominal acceleration environment. A fixed control schemethat can handle these impulses produces gyroscope disturbance torques far in excess of mission requirements.An adaptive Linear Quadratic Estimator (LQE) control algorithm has been developed to meet the high dynamicrange requirements for the mission’s electrostatic suspension. The controller architecture is novel because ituses estimates of the plant’s state, rather than estimates of the plant’s parameters, as inputs for adaptation(Figure 9-8). This allows the algorithm to dynamically increase its control authority and bandwidth to the levelneeded to respond to large impulsive disturbances while continuously minimizing control authority - andtorques - during nominal operation. The net result of this scheme is that the control system performs like ahigh-bandwidth and high authority controller with respect to disturbances that move the rotor far from thecommanded position, but performs like a low-bandwidth, low-authority control system with respect togyroscope disturbance torques. Figure 9-9 shows the simulated response to variously sized micrometeoroids;this performance has been verified in orbit. This variable bandwidth control scheme, in part, allows the <strong>GP</strong>-Bmission achieve its goal for the non-relativistic residual gyroscope precession rate of less than 1.6×10 11 deg/hr.<strong>Gravity</strong> <strong>Probe</strong> B — <strong>Post</strong> <strong>Flight</strong> Analysis • Final <strong>Report</strong> March 2007 263

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