Elsevier

Mechanism and Machine Theory

Volume 104, October 2016, Pages 350-369
Mechanism and Machine Theory

Dynamic modeling and control of a 6-DOF micro-vibration simulator

https://doi.org/10.1016/j.mechmachtheory.2016.06.011Get rights and content

Highlights

  • A 6 degree-of-freedom (DOF) micro-vibration simulator (6-MVS) is proposed.

  • The dynamics equations, which consider the effect of the flexure joints, are derived.

  • A robust proportional-integral control scheme is carried out.

Abstract

A micro-vibration simulator with multiple degrees of freedom is required for performance testing of sensitive instruments in a micro-vibration environment on-board spacecraft before launch. In this study, a novel 6-DOF micro-vibration simulator (6-MVS) is proposed, which can reproduce a micro-vibration environment with a wide bandwidth of disturbance frequencies. The complete inverse dynamic equations of the proposed 6-MVS are derived using the Kane method, which is very suitable for processing by computer. The validity of the derived dynamic equations is then verified by co-simulation. The structural performance of the 6-MVS is investigated using the finite element method. Based on this dynamic model, a robust proportional-integral (PI) control scheme is then performed. The control performance of the proposed controller is evaluated by co-simulation. The analysis and simulation results show that the proposed robust PI controller has excellent robustness and stability and the 6-MVS can exactly produce the required micro-vibration spectrum.

Introduction

There is an increasing requirement for precision pointing and extreme stability for current and forthcoming optical remote sensors, which have a larger aperture and a higher resolution imaging. The James Webb space telescope [1], terrestrial planet finder [2] and Space Interferometry Mission [3] are such examples where microarcsecond pointing and nanometer levels of motion stability are required. However, micro-vibrations generated by on-board motion equipment in spacecraft (for example, reaction/momentum wheel assemblies (R/MWA), cryo-coolers, thrusters, solar array drive mechanisms, etc.) can greatly degrade the performance of optical payloads with high pointing accuracy and stability [4].

Since micro-vibrations have characteristics of low amplitude, a wide frequency range, and multiple directions, current shake tables are unable to reproduce the required micro-vibration environment. Hostens et al. [5, 6] have proposed a six degree-of-freedom (DOF) vibration simulator, which can be used to generate high-amplitude and narrow-band vibrations. Park et al. [7] have developed a multiple-degree-of-freedom micro-vibration emulator to test jitter in spacecrafts, which can generate the disturbance spectrum of flight RWAs. However, this device has some coupling effects causing differences between the target input and the measured data responses along different axes. For space payloads, ground experiments are essential before launch, including image quality testing of the optical system in the micro-vibration environment. However, no suitable micro-vibration simulator exists that is qualified for this work. The usual solution is to adopt the actual disturbance resources or use dummy resources in the ground experiments. The R/MWA is generally regarded as one of the largest disturbance sources onboard a spacecraft [8]. Therefore, a real R/MWA is usually used for the micro-vibration test. However, it is uncommon to use all the flight R/MWAs to conduct the ground validating experiments because of scheduling issues or product assurance activities. Therefore, development of a micro-vibration shaking platform, which can replace the real flight R/MWAs, is considered to be an important adjunct to the development processes for space missions.

Parallel manipulators such as the Gough-Stewart platform (GSP) have been recently employed in various applications, because they have the advantages of high maneuverability, precision, high stiffness, and a large payload driven capability compared with serial manipulators. Li and Xu [9] have presented a three-prismatic-revolute-cylindrical parallel kinematic machine, and have investigated its dynamic modeling and robust control. A six degree-of-freedom parallel kinematic machine has been developed by Dong et al. [10], which is used for the motion simulation of hazardous chemical transportation. The Gough-Stewart platform, also known as the hexapod, is one of the most widely used parallel manipulators [11], [12], [13], [14], [15]] and its kinematics, dynamics and control problems have been studied by many researchers. Oftadeh et al. [16] have presented explicit dynamics formulation for the GSP and utilized the Lagrange method to verify the resulting dynamics equations. Dasgupta and Mruthyunjaya [17] have derived an inverse dynamic formulation using the Newton-Euler approach for the GSP, with frictional forces occurring in the joints; the mass of inertia of the pods was also taken into consideration in their study. Staicu [18, 19] has developed a recursive matrix approach in kinematics and dynamics modeling of parallel robots, which can reduce the number of equations and computation operations significantly. Jiang et al. [20], [21], [22], [23], [24]] have investigated an optimal design of the GSP with dynamic isotropy, as well as the influence of passive joint damping. Behrouz et al. [25] have developed a full parameter model of the GSP damped vibrations, which includes parametric expressions of the damped eigenfrequencies and the corresponding eigenvectors.

The control strategies for the parallel manipulator can be divided into two categories: control in the joint space and control in the task space [26]. The former control scheme can be readily employed in industry, but does not always guarantee high performance for parallel manipulators [27]. Kim et al. [28] have proposed a robust nonlinear control scheme in the joint space for an electro-hydraulic parallel manipulator based on the Lyapunov redesign method, but coupling is not taken into account, which should not be ignored for high performance tracking controllers. Wu et al. [29] presented an improved robust nonlinear controller, which is composed of the linear control part, nonlinear part and excitation compliment part. This proposed controller has the advantages of fine adjustability, low power consumption and a wide frequency range of isolation in all directions. But its pivotal objective is to attenuate the micro-vibrations. Superior control performance can potentially be provided using the control scheme in the task space. Han et al. have published a series of reports on robust controls for 6-DOF parallel manipulators, which include a computed force and velocity control, proportional plus derivative control and decoupling control schemes, etc. [30], [31], [32], [33], [34]]. Kim et al. [35] have proposed a robust nonlinear task space control with a friction estimator for a dynamoelectric GSP. However, most studies have focused mainly on displacement or velocity trajectory tracking control, while acceleration trajectory tracking control of a parallel manipulator with multiple degrees of freedom is still rare. Although some acceleration trajectory control strategies have by been reported in Refs. [36, 37], they are only suitable for shake tables with a single degree of freedom.

In this study, a 6-DOF micro-vibration simulator (6-MVS) has been developed, which can reproduce micro-vibrations with different amplitudes and frequencies. While a conventional GSP has stretched rods, the structural configuration of the proposed 6-MVS has been improved and has rods of fixed length. Since the mass of the rods in a conventional GSP is relatively heavy, a GSP may have low and closely-spaced local natural frequencies [38]. As a result, the natural frequencies of the overall system are reduced. The improved configuration simulator that is presented in this study can solve this problem, and its structural characteristics have been analyzed using the finite element method (FEM). Moreover, flexure joints are adopted to avoid nonlinear effects due to friction, backlash, and micro-impacts which are produced by traditional joints with bearings. The inverse dynamics models, which consider the effect of the flexure joints, were established using the Kane method. A co-simulation was then adopted to verify the validity of the dynamics models, which combined ADAMS with MATLAB/Simulink. Finally, a robust proportional-integral (PI) controller based on the inverse dynamics model was designed. This control strategy was designed for the acceleration control of the parallel manipulator, which considered the effects of uncertainties such as modeling errors, unknown loads, and parameter measurements. Its performance was analyzed in theory and simulation, including stability, precision and robustness of the proposed controller.

Section snippets

Mechanical structure

A virtual prototype of the 6-DOF micro-vibration simulator is shown in Fig. 1. The 6-MVS consists of an upper platform, a base platform, three fixed mounts and six identical legs. The detailed structure of the leg is depicted in Fig. 2, which includes an actuator, a rod and two flexure joints. The actuator is attached to a fixed mounting by bolts. A permanent magnet is fixed to the cover of the actuator, and a voice coil is connected to the cover by two membranes. The two membranes perform the

Dynamic model

Nomenclature

    PBR

    rotation matrix of transformation from the body frame {P} to the base frame {B}

    Jpi,q

    Jacobian matrix relating the general velocity to the velocity of the upper flexure joint

    Jd,q

    Jacobian matrix relating the general velocity to the sliding velocity of the actuator

    E3

    unit 3 × 3 matrix

    α, β, γ

    X-Y-Z fixed angles

    Q1si,Q2si,Q1pi,Q2pi,Q3pi

    Z-Y-X Euler angles of successive rotation

    s^3i,d^3i

    unit vectors along the ith rod and actuator, respectively

    si , di

    lengths of the ith rod and actuator,

Finite element analysis

In this paper, the dynamic model of the mechanical system for the parallel robot is viewed as thirteen rigid bodies. However, when there are high-frequency exciting forces acting on an actual system, elastic deformations need to be taken into account. The results of mode analysis characterize the basic dynamic behavior of the structure and are an indication of how the structure will respond to dynamic loading. Therefore, the finite element method is adopted to analyze the normal mode of the

Dynamic model verification

The main objective of the proposed inverse dynamic model is to compute the required actuator forces when given the desired accelerations at different frequencies. However, the accuracy and effectiveness of the developed dynamic model have not yet been verified. In this section, a co-simulation using ADAMS and MATLAB/Simulink has been adopted to verify the validity of the dynamic model and the feasibility of the 6-MVS. The MATLAB/Simulink environment is used to compute the required actuator

Control strategy and simulation

The model implemented in Section 5 is an ideal model. However, since an actual 6-MVS will not exactly coincide with the theoretical model, a control measure needs to be implemented for the 6-MVS. The classical computed torque control (CTC) approach uses an inverse dynamic model to decouple and linearize the nonlinear dynamics of the parallel manipulator. Therefore, if the dynamic model is accurate enough, the resulting system will be a series of decoupled linear systems that can be easily

Conclusion

This study presents the structural design, inverse dynamics modeling, and robust control of a micro-vibration simulator, which can reproduce 6-DOF micro-vibrations with different amplitudes and frequencies. The Kane method is used to establish a complete inverse dynamics model of the 6-DOF micro-vibration simulator (6-MVS), where the parallel manipulator is considered to be a multiple-rigid-body system. This derived dynamics model takes the effects of the flexure joint into account. The finite

Acknowledgments

This work was supported by the National Natural Science Foundation of China under Grant no. 11302222 and the Innovation Foundation of Changchun Institute of Optics, Fine Mechanics and Physics, Chinese Academy of Sciences under Grant no. Y4CX1SS141.

References (39)

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