Attitude Maneuvering Control Method for Flexible Satellite Based on Tracking Time-Energy Optimal Trajectory
A technology for tracking time and flexible satellites, applied in three-dimensional position/channel control and other directions, it can solve the problems of poor robustness and high energy consumption of the flywheel, and achieve good robustness, complete robustness, and energy saving. consumption effect
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specific Embodiment approach 1
[0035] Specific implementation mode one: combine figure 1 This implementation is described, based on the tracking time-energy optimal trajectory control method for flexible satellite attitude maneuvering. It includes the following steps:
[0036] Step 1: Use x-y-z sequence Euler angles to describe the satellite attitude, establish the dynamics and kinematics equations of the satellite, ignore the influence of flexibility factors under the premise of reasonable bandwidth design, and simplify the dynamic model of the flywheel as the actuator, Design a nonlinear decoupled torque controller;
[0037] Step 2: Under the premise that the initial attitude angle, initial attitude angular velocity, target attitude angle, target attitude angular velocity, moment of inertia and output torque amplitude are given, according to the time-energy optimal control method, starting from the moment of maneuvering, real-time Calculate an optimal angle tracking trajectory and its corresponding op...
specific Embodiment approach 2
[0039] Specific implementation mode two: the specific operation steps of step 1 of this embodiment mode are:
[0040] For a wheel-controlled spacecraft with a flexible solar sail, considering the influence of the disturbance moment, the attitude dynamic equation and the sail flexible vibration equation are:
[0041]
[0042] where I s =diag(I x ,I y ,I z ) is the moment of inertia matrix of the spacecraft, Ix is the moment of inertia of the spacecraft about the x-axis of the system, I y is the moment of inertia of the spacecraft about the y-axis of the system, I z is the moment of inertia of the spacecraft about the z-axis of the system, ω s =[ω x ,ω y ,ω z ] T is the component matrix of the inertial angular velocity vector of the spacecraft in this system, for ω s Derivative with respect to time, T c and T d are the control torque and external disturbance torque vectors, respectively. η,ε,Ω,F s Corresponding to the flexible mode coordinates of the sailboard...
specific Embodiment approach 3
[0064] Specific implementation mode three: the specific operation steps of step 2 of this embodiment mode are:
[0065] Time-energy optimal control is the weighting of time optimal control and energy optimal control, that is,
[0066]
[0067] Among them, ρ≥0 is the time weighting coefficient, indicating the designer’s emphasis on the response time; if ρ=0, it means that the response time is ignored, and only the most energy consumption is considered; if ρ=∞, it means that the energy consumption is not considered Consumption, only requires the shortest time. tf is the maneuvering time, u(t) is the torque output by the flywheel; starting from step 2, and represent the same variable;
[0068] Let the initial value of the angle at the beginning of the maneuver be The angular velocity is 0, and the target maneuvering angle is The target maneuvering angular velocity is 0, and the moment of inertia is I x , the output torque amplitude is u x , and the weighted time coe...
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Abstract
Description
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Application Information
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