全部 标题 作者
关键词 摘要

OALib Journal期刊
ISSN: 2333-9721
费用:99美元

查看量下载量

相关文章

更多...

Optimal Manoeuvres of Underactuated Linear Mechanical Systems: The Case of Controlling Gantry Crane Operations

DOI: 10.1155/2014/283565

Full-Text   Cite this paper   Add to My Lib

Abstract:

A method of solving optimal manoeuvre control of linear underactuated mechanical systems is presented. The nonintegrable constraints present in such systems are handled by adding dummy actuators and then by applying Lagrange multipliers to reduce their action to zero. The open- and closed-loop control schemes can be analyzed. The method, referred to as the constrained modal space optimal control (CMSOC), is illustrated in the examples of gantry crane operations. 1. Introduction Underactuated mechanical systems have fewer independent actuators than degrees of freedom (DOFs) to be controlled [1]. Typical nonlinear examples of such systems, usually with only several DOFs, are rigid multilink robotic manipulators with passive joints or any manipulator with flexible links (described by at least one mode of vibration). Linear examples include vibrating structures with continuously distributed mass (i.e., with theoretically infinite number of DOFs to describe them) such as masts, antennas, buildings, brides, and car suspension, controlled by discrete actuators. This paper presents a method of analyzing and simulating optimal manoeuvres between two given configurations (often referred to as point-to-point manoeuvres) for linear underactuated systems. The method combines optimal control theory with computational mechanics and the finite element (FE) technique, in particular. The number of DOFs equal to the number of actuators will be referred to as actuated (after [1]), while all remaining DOFs will be referred to as underactuated (however, all DOFs are in fact controlled). The actuated and unactuated DOFs must satisfy a number of constraints equal to the number of unactuated DOFs and resulting from the equations governing the motion of such systems. For mechanical systems we assume that these constraints may be nonintegrable (nonholonomic), meaning unactuated DOFs cannot be explicitly eliminated. Many of the techniques presented in the literature deal with underactuated problems by applying the constraints to eliminate the unactuated DOFs and then by solving the reduced fully actuated problems [2–4]. These approaches are limited to particular problems where the constraints can be simplified to a form making such mathematical manipulations possible. The method presented here is capable of dealing with any linear system, as it does not require the elimination of unactuated DOFs. Instead, the underactuated system is formulated as if it were fully actuated by adding “dummy” (zero-valued) actuators to all unactuated DOFs. The modal space is used in modelling the

References

[1]  I. Fantoni and R. Lozano, Non-Linear Control for Underactuated Mechanical Systems, Springer, 2002.
[2]  L. Meirovitch and H. Baruh, “Control of self-adjoint distributed-parameter systems,” Journal of Guidance, Control, and Dynamics, vol. 5, no. 1, pp. 60–66, 1982.
[3]  B. L. Karihaloo and R. D. Parbery, “Optimal control of a dynamical system representing a gantry crane,” Journal of Optimization Theory and Applications, vol. 36, no. 3, pp. 409–417, 1982.
[4]  M. W. Spong, “The swing up control problem for the acrobot,” IEEE Control Systems Magazine, vol. 15, no. 1, pp. 49–55, 1995.
[5]  R. A. Canfield and L. Meirovitch, “Integrated structural design and vibration suppression using independent modal space control,” AIAA Journal, vol. 32, no. 10, pp. 2053–2060, 1994.
[6]  R. Seifried, “Two approaches for feedforward control and optimal design of underactuated multibody systems,” Multibody System Dynamics, vol. 27, no. 1, pp. 75–93, 2012.
[7]  R. Seifried and W. Blajer, “Analysis of servo-constraint problems for underactuated multibody systems,” Mechanical Sciences, vol. 4, pp. 113–129, 2013.
[8]  W. Blajer and K. Ko?odziejczyk, “Control of underactuated mechanical systems with servo-constraints,” Nonlinear Dynamics, vol. 50, no. 4, pp. 781–791, 2007.
[9]  W. Blajer and K. Ko?odziejczyk, “A geometric approach to solving problems of control constraints: theory and a DAE framework,” Multibody System Dynamics, vol. 11, no. 4, pp. 343–364, 2004.
[10]  M. Fliess, J. Lévine, P. Martin, and P. Rouchon, “Flatness and defect of non-linear systems: introductory theory and examples,” International Journal of Control, vol. 61, no. 6, pp. 1327–1361, 1995.
[11]  H. Sira-Ramirez and S. K. Agrawal, Differentially Flat Systems, Control Engineering Series, Marcel Dekker, 2004.
[12]  K. -J. Bathe, “Modal superposition,” in Finite Elements Procedures, chapter 9.3, Prentice Hall, Englewood Cliffs, NJ, USA, 1996.
[13]  S. Woods and W. Szyszkowski, “Simulating active vibration attenuation in underactuated spatial structures,” Journal of Guidance, Control, and Dynamics, vol. 32, no. 4, pp. 1246–1253, 2009.
[14]  S. Woods and W. Szyszkowski, “Analysis and simulation of optimal vibration attenuation for underactuated mechanical systems,” AIAA Journal, vol. 47, no. 12, pp. 2821–2835, 2009.
[15]  D. E. Kirk, Optimal Control Theory, Dover, New York, NY, USA, 1998.
[16]  D. G. Zill and M. R. Cullen, Advanced Engineering Mathematics, PWS Publishing Company, Boston, Mass, USA, 1992.
[17]  E. M. Abdel-Rahman, A. H. Nayfeh, and Z. N. Masoud, “Dynamics and control of cranes: a review,” Journal of Vibration and Control, vol. 9, no. 7, pp. 863–908, 2003.
[18]  H.-H. Lee, “Modeling and control of a three-dimensional overhead crane,” Journal of Dynamic Systems, Measurement and Control, vol. 120, no. 4, pp. 471–476, 1998.
[19]  W. O. Connor and H. Habibi, “Gantry crane control of a double-pendulum, distributed-mass load, using mechanical wave concept,” Mechanical Sciences, vol. 4, pp. 251–261, 2013.

Full-Text

Contact Us

service@oalib.com

QQ:3279437679

WhatsApp +8615387084133