1964
DOI: 10.1002/j.1538-7305.1964.tb04104.x
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Attitude Determination and Prediction of Spin-Stabilized Satellites

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Cited by 11 publications
(3 citation statements)
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“…where I z is the moment of inertia along the spin axis, N x , N y , N z are the components of the external torques in the body system and here are given by the sum of the mean components of gravity gradient, aerodynamic, solar radiation, residual magnetic and eddy current torques. The analytical approach for this case is similar to that of Thomas and Cappelare (1964) and Yu (1963). Applications in these references were done for the Telstar satellites using the magnetics torque with dipolo model for the geomagnetic field.…”
Section: Analytical Approachmentioning
confidence: 91%
“…where I z is the moment of inertia along the spin axis, N x , N y , N z are the components of the external torques in the body system and here are given by the sum of the mean components of gravity gradient, aerodynamic, solar radiation, residual magnetic and eddy current torques. The analytical approach for this case is similar to that of Thomas and Cappelare (1964) and Yu (1963). Applications in these references were done for the Telstar satellites using the magnetics torque with dipolo model for the geomagnetic field.…”
Section: Analytical Approachmentioning
confidence: 91%
“…These components are obtained in terms of the geocentric inertial components of the geomagnetic field (Thomas and Cappelari, 1964) and the attitude quaternion of the satellite . In order to describe the geomagnetic field, the dipole vector model (Thomas and Cappelari ,1964;Zanardi et al, 2005) is used.…”
Section: Magnetic Torquesmentioning
confidence: 99%
“…The geomagnetic field is described by the dipole vector model (Thomas and Cappelari ,1964;Zanardi et al, 2005).…”
Section: Torque Due Lorentz Forcementioning
confidence: 99%