1993
DOI: 10.2514/3.21060
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Pointing accuracy of a dual-spin satellite due to torsional appendage vibrations

Abstract: This paper deals with the attitude motion of a dual-spin satellite with a finite sized rigid body attached to the end of a flexible beam. The equations of motion are derived using Lagrange's equations and are solved using the perturbation technique known as the Krylov-Bogoliubov-Mitropolsky method. The special case of torsional flexibility is presented in its entirety. The relationships between the satellite, beam and tip mass parameters, and pointing accuracy of the satellite are examined.

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Cited by 6 publications
(4 citation statements)
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“…where u> 2 = cos# -<w z sin0), [a> y + 6(L,t)] 9 (co z cos# -co x sin 0)} is the angular velocity of the tip mass expressed in terms of principal coordinates of the tip mass, and/ 2 = diag[/ x , I y , I z ] is the principal inertia tensor of the tip mass about c 2 . It is also diagonal relative to the xyz frame in the undeformed case.…”
Section: Problem Formulation and Equations Of Motion Satellite Modelmentioning
confidence: 99%
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“…where u> 2 = cos# -<w z sin0), [a> y + 6(L,t)] 9 (co z cos# -co x sin 0)} is the angular velocity of the tip mass expressed in terms of principal coordinates of the tip mass, and/ 2 = diag[/ x , I y , I z ] is the principal inertia tensor of the tip mass about c 2 . It is also diagonal relative to the xyz frame in the undeformed case.…”
Section: Problem Formulation and Equations Of Motion Satellite Modelmentioning
confidence: 99%
“…Note that the method of averaging is applied twice in this process, first in order to obtain the T = 0 solution from Ref. 9 and then to obtain the slow evolution of energy (as in this work). In each case, a small parameter is available to justify the use of the averaging approximation.…”
Section: Introductionmentioning
confidence: 99%
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