A Method of Attitude Control for Magnetron Bias Momentum Satellite Based on Periodic Lyapunov Equation
A technology of bias momentum and attitude control, applied in attitude control, adaptive control, general control system, etc. Saturation and other issues
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specific Embodiment approach 1
[0042] Specific embodiment one: the attitude control method of a kind of magnetron bias momentum satellite based on period Lyapunov equation of the present embodiment, specifically realize according to the following steps:
[0043] Step 1: Establish the satellite body coordinate system with the satellite center of mass as the origin o, fix the x, y and z axes on the satellite body, according to ω x , ω y , ω z Establish the linearized dynamic model of the magnetron bias momentum satellite, that is, the attitude dynamic equation of the bias momentum satellite; where the x-axis points forward along the longitudinal symmetry axis of the satellite, and the y-axis points downward perpendicular to the x-axis in the longitudinal symmetry plane of the satellite , the z-axis is perpendicular to the oxy plane, the direction of the z-axis follows the right-hand spiral rule, the x-axis is the roll axis, the y-axis is the pitch axis and the z-axis is the yaw axis; ω x , ωy , ω z is the ...
specific Embodiment approach 2
[0058] Specific embodiment two: the difference between this embodiment and specific embodiment one is that in step one, the satellite body coordinate system is established with the center of mass of the satellite as the origin o, and the x, y and z axes are fixed on the satellite body, according to ω x , ω y , ω z The specific process of establishing the linearized dynamic model of the magnetron bias momentum satellite, that is, the attitude dynamic equation of the bias momentum satellite, is as follows:
[0059] I ω · + ω × ( Iω + h ) = - h · + T
[0060] In the formula, ω=[ω x ω y ω z ] T is the rotational angular velocity of the satellite body coordinate system relative to the geocentric inertia coordinate system, is the change rate of...
specific Embodiment approach 3
[0093] Specific embodiment three: what this embodiment is different from specific embodiment one or two is: select design parameter γ in step 2, i.e. scalar function γ, the specific process of solving periodic Lyapunov differential equation is:
[0094] (1), the periodic Lyapunov differential equation is:
[0095] W · ( t ) = W ( t ) A T + AW ( t ) + γ ( t ) W ( t ) - B ( t ) R - 1 ( t ) B T ...
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