Abstract

The novel contribution in this manuscript is an expansion of the current state-of-the-art in the geometric installation of control moment gyroscopes beyond the benchmark symmetric skewed arrays and the four asymmetric arrays presented in recent literature. The benchmark pyramid symmetrically skewed at 54.73 degrees mandates significant attention to singularity avoidance, escape, and penetration, while the most recent four asymmetric arrays are strictly useful in instances where space is available to mount at least one gyro orthogonal to the others. Skewed arrays of gyros and the research-benchmark are introduced, followed by the present-day box-90 and “roof” configurations, where the roof configuration is the first prevalently used asymmetric geometry. Six other asymmetric options in the most recent literature are introduced, where four of the six options are obviously quite useful. From this inspiration, several dozen discrete options for asymmetric installations are critically evaluated using two figures of merit: maximum momentum (saturation) and maximum singularity-free momentum. Furthermore, continuous surface plots are presented to provide readers with countless (infinite) options for geometric installations. The manuscript firmly establishes many useful options for engineers who learn that the physical space on their spacecraft is insufficient to permit standard installations.

Highlights

  • Motion mechanics is governed by Euler’s moment equations for three degrees of rotation of rigid bodies in space [1], and Newton’s Law [2] for three dimensions of translation

  • Rigid body motion mechanics governing spacecraft attitude control has a long, distinguished lineage of literature [3,4,5,6,7,8,9,10,11,12,13,14,15,16,17] that has culminated in recent advances using the governing Euler’s moment equations as the control [18,19,20,21,22,23,24,25,26,27] in a scheme called deterministic artificial intelligence [28,29]

  • This study will be limited to non-redundant, constant-speed, single-gimbaled control moment gyroscopes (CMGs)

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Summary

Introduction

Motion mechanics is governed by Euler’s moment equations for three degrees of rotation of rigid bodies in space [1], and Newton’s Law [2] for three dimensions of translation. Rigid body motion mechanics governing spacecraft attitude control has a long, distinguished lineage of literature [3,4,5,6,7,8,9,10,11,12,13,14,15,16,17] that has culminated in recent advances using the governing Euler’s moment equations as the control [18,19,20,21,22,23,24,25,26,27] in a scheme called deterministic artificial intelligence [28,29]. Gyros use a relationship called a steering law [31,32,33,34,35,36] to calculate gyro commands for designed changes in angular momentum (torque commands generated by attitude controllers to accomplish a desired maneuver). Engineers design maneuvers in such a manner so that they never demand torque that would produce an angular momentum trajectory that is required to pass through

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