Spacecraft rendezvous fault diagnosis and filter design method based on event driving
A filter design and event-driven technology, which is applied in the fields of instrumentation, computing, and electrical digital data processing, etc., can solve the problems of high energy consumption in data transmission and high bus bandwidth occupancy
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specific Embodiment approach 1
[0032] Specific implementation mode 1: The specific process of the event-driven spacecraft rendezvous fault diagnosis and filter design method in this implementation mode is as follows:
[0033] Step 1. The orbital coordinate system of the tracker and the target spacecraft is as follows: figure 1 As shown, according to Newton's dynamics theory, the C-W equation is established, and the state-space model of the spacecraft rendezvous system is established according to the kinematic equation;
[0034] Step 2, designing a weighted fault function to improve fault diagnosis performance;
[0035] Step 3. Based on the state space model of the spacecraft rendezvous system established in step 1, design a gain matrix based on dynamic event-driven FDF, and establish an augmented residual system under event-driven conditions;
[0036] Step 4. According to the gain matrix of FDF, get and x(t), then according to And u(t)=Kx(t), get residual signal r(t) and control input u(t);
[0037] ...
specific Embodiment approach 2
[0042] Specific embodiment 2: The difference between this embodiment and specific embodiment 1 is that the orbital coordinate system between the tracker and the target spacecraft in the step 1 is as follows figure 1 As shown, according to the Newtonian dynamics theory, the C-W equation is established, and the state-space model of the spacecraft rendezvous system is established according to the kinematic equation; the specific process is:
[0043] According to Newton's dynamics theorem, the relative dynamics model of the spacecraft is as follows:
[0044]
[0045]
[0046]
[0047] Among them, x, y, z are the relative position components in the satellite orbit coordinate system; Respectively, the relative velocity components of the x-axis, y-axis, and z-axis of the satellite orbit coordinate system; r 0 is the center distance of the target aircraft; μ e is the gravitational constant of the earth; n is the orbital angular velocity of the target aircraft, equal to ...
specific Embodiment approach 3
[0058] Specific embodiment three: the difference between this embodiment and specific embodiment one or two is that the spacecraft rendezvous system matrix A 0 , B 0 , B 1 , the C expression is as follows:
[0059]
[0060]
[0061] Other steps and parameters are the same as those in Embodiment 1 or 2.
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