In order for Active Debris Removal to be accomplished, it is critically important to understand the probable rotation states of orbiting, spent rocket bodies. As compared to the question of characterizing small unresolved debris, in this problem there are several advantages: (1) objects are of known size, mass, shape and color, (2) they have typically been in orbit for a known period of time, (3) they are large enough that resolved images may be obtainable for verification of predicted orientation, and (4) the dynamical problem is simplified to first order by largely cylindrical symmetry. It is also nearly certain for realistic rocket bodies that internal friction is appreciable in the case where residual liquid or, to a lesser degree, unconsolidated solid fuels exist. Equations of motion have been developed for this problem in which internal friction as well as torques due to solar radiation, magnetic induction, and gravitational gradient are included. In the case of pure cylindrical symmetry, the results are compared to analytical predictions patterned after the standard approach for analysis of symmetrical tops. This is possible because solar radiation and gravitational torques may be treated as conservative. Agreement between results of both methods ensures their mutual validity. For monotone symmetric cylinders, solar radiation torque vanishes if the center of mass resides at the geometric center of the object. Results indicate that in the absence of solar radiation effects, rotation states tend toward an equilibrium configuration in which rotation is about the axis of maximum inertia, with the axis of minimum inertia directed toward the center of the earth. Solar radiation torque introduces a modification to this orientation. The equilibrium state is asymptotically approached within a characteristic timescale given by a simple ratio of relevant characterizing parameters for the body in question. Light curves are simulated for the expected asymptotic final rotation states of model objects, and these are compared to data derived from physical models of the same objects, tested in the Optical Measurements Center at JSC. Comparison to relevant light curves from actual orbiting rocket bodies are also performed, and diagnostic features of such curves are examined.
[1]
J.-C. Liou,et al.
Optical Signature Analysis of Tumbling Rocket Bodies via Laboratory Measurements
,
2012
.
[2]
J. Liou.
An active debris removal parametric study for LEO environment remediation
,
2011
.
[3]
Moriba Jah,et al.
Attitude Determination from Light Curves
,
2009
.
[4]
T. Yanagisawa,et al.
Shape and Motion Estimate of LEO Debris Using Light Curves
,
2007
.
[5]
J. Vanyo.
Rotating Fluids in Engineering and Science
,
1993
.
[6]
A. J. Meadows,et al.
Eddy current torques, air torques, and the spin decay of cylindrical rocket bodies in orbit
,
1978
.
[7]
G. Smith.
Effects of magnetically induced eddy-current torques on spin motions of an earth satellite
,
1965
.
[8]
Moriba K. Jah,et al.
Satellite Characterization: Angles and Light Curve Data Fusion for Spacecraft State and Parameter Estimation
,
2007
.
[9]
A. P. Torzhevskii.
Rapid Spinning of an Artificial Satellite about its Center of Mass in Resonance
,
1968
.
[10]
G. Smith.
A Theoretical Study of the Torques Induced by a Magnetic Field on Rotating Cylinders and Spinning Thin-wall Cones, Cone Frustums, and General Body of Revolution
,
1962
.