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Structure of the solar array system

Structure of the solar array system

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It is well known that the traditional modeling theories adopt the Cartesian coordinates to establish the dynamic equation of solar array system. The order of this equation is often very high, which is inconvenient for controller design. The Cartesian coordinates are difficult to be measured in practice. In this paper, the joint coordinates are used...

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... 7 Moreover, the motion forms of the space structure are also complex and diverse when they are in large scales, such as large maneuvering, [8][9][10] space movement of large manipulator, [11][12][13] rendezvous and docking, [14][15][16] and large-scale appendage deployment and locking. [17][18][19] For example, the flexible vibration of the solar panels poses a strong coupling effect on the attitude of the spacecraft body and the joint motion of the robotic arm for large or substantially large spacecraft platforms with enormous flexible solar panels, such as GEO communication satellites. 20 Therefore, these problems cannot ignore the influence of structural deformation or vibration characteristics. ...
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... Therefore, the considered two-dimensional approach will be incorrect. In a real situation, many characteristic sizes of the solar panels of various small spacecrafts allow us to neglect transverse oscillations compared with longitudinal ones [18,23]. Therefore, this hypothesis has a basis. ...
... Taking into account the expression for temperature (20) and derivative (22), Equation (23) can be rewritten as follows: ...
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... Li et al. [22] investigated the coupling effects of joint clearance and panel flexibility on the overall dynamic characteristics of a deployable solar array system. Li et al [23,24] established the dynamic equation of the solar array system by using single direction recursive construction method and the Jourdain's velocity variation principle to study the deployment and control of flexible solar array system considering joint friction. Furthermore, Li et al. [25] established the rigid-flexible coupling dynamics model of deployable solar array system with multiple clearance joints based on nodal coordinate formulation (NCF) and absolute nodal coordinate formulation (ANCF) to analyze and control satellite attitude under deployment disturbance, and presented significant guidance for the key parameters design of torsional spring, closed cable loops (CCL) configuration, and latch mechanism [26]. ...
... A BISTOP function is introduced to present the equivalent moment T lock in the latch mechanism [23][24][25][26]. BISTOP function allows free motion between x 1 and x 2 at which point the contact function begins to push the joint back toward the expect center angle. ...
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... A novel computational approach for modeling and analysis of a spacecraft with symmetric flexible solar arrays within the framework of global analytical modes was proposed [16][17][18][19] . Li et al. [20][21][22][23] investigated the deployment dynamics of a spacecraft solar array system with joint friction and developed a fuzzy proportional derivative (PD) controller to eliminate the drift of the base spacecraft. ...
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A control strategy combining feedforward control and feedback control is presented for the optimal deployment of a spacecraft solar array system with the initial state uncertainty. A dynamic equation of the spacecraft solar array system is established under the assumption that the initial linear momentum and angular momentum of the system are zero. In the design of feedforward control, the dissipation energy of each revolute joint is selected as the performance index of the system. A Legendre pseudospectral method (LPM) is used to transform the optimal control problem into a nonlinear programming problem. Then, a sequential quadratic programming algorithm is used to solve the nonlinear programming problem and offline generate the optimal reference trajectory of the system. In the design of feedback control, the dynamic equation is linearized along the reference trajectory in the presence of initial state errors. A trajectory tracking problem is converted to a two-point boundary value problem based on Pontryagin’s minimum principle. The LPM is used to discretize the two-point boundary value problem and transform it into a set of linear algebraic equations which can be easily calculated. Then, the closed-loop state feedback control law is designed based on the resulting optimal feedback control and achieves good performance in real time. Numerical simulations demonstrate the feasibility and effectiveness of the proposed control strategy.
... Considering panel flexibility and multiple clearance joints, Li et al. [49,50] further studied dynamics of deployable solar array system with multiple clearance joints and given some design suggestions of the whole system by using commercial software ADAMS. Hai-Quan Li et al. [51] study the deployment and control of flexible solar array system considering joint friction without normal contact force. However, to study the effects of joint clearance on attitude of solar array system with flexible panels, considering both contact force and friction force, is still insufficient. ...
... The BISTOP function allows free motion between x 3 and x 4 at which point the contact function begins to push the joint back towards the expect center angle. The specific details are set referencing literature [5,51,52]. ...
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Based on Nodal Coordinate Formulation (NCF) and Absolute Nodal Coordinate Formulation (ANCF), this paper establishes rigid-flexible coupling dynamic model of the spacecraft with large deployable solar arrays and multiple clearance joints to analyze and control the satellite attitude under deployment disturbance. Considering torque spring, close cable loop (CCL) configuration and latch mechanisms, a typical spacecraft composed of a rigid main-body described by NCF and two flexible panels described by ANCF is used as a demonstration case. Nonlinear contact force model and modified Coulomb friction model are selected to establish normal contact force and tangential friction model, respectively. Generalized elastic force are derived and all generalized forces are defined in the NCF-ANCF frame. The Newmark-β method is used to solve system equations of motion. The availability and superiority of the proposed model is verified through comparing with numerical co-simulations of Patran and ADAMS software. The numerical results reveal the effects of panel flexibility, joint clearance and their coupling on satellite attitude. The effects of clearance number, clearance size and clearance stiffness on satellite attitude are investigated. Furthermore, a proportional-differential (PD) attitude controller of spacecraft is designed to discuss the effect of attitude control on the dynamic responses of the whole system.