A STRUCTURAL FLEXIBILITY TRANSFORMATION MATRIX FOR MODELING OPEN-KINEMATIC CHAINS WITH REVOLUTE AND PRISMATIC JOINTS

Citation
Ng. Chalhoub et L. Chen, A STRUCTURAL FLEXIBILITY TRANSFORMATION MATRIX FOR MODELING OPEN-KINEMATIC CHAINS WITH REVOLUTE AND PRISMATIC JOINTS, Journal of sound and vibration, 218(1), 1998, pp. 45-63
Citations number
18
Categorie Soggetti
Acoustics
ISSN journal
0022460X
Volume
218
Issue
1
Year of publication
1998
Pages
45 - 63
Database
ISI
SICI code
0022-460X(1998)218:1<45:ASFTMF>2.0.ZU;2-Y
Abstract
A general approach to systematically derive the equations of motion of flexible open-kinematic chains is presented in this paper. The method ology exploits the serial characteristic of the kinematic chain by com plementing the. 4 x 4 Denavit-Hartenberg transformation matrix with a 4 x 4 structural flexibility matrix. The latter is defined based on a floating coordinate system which rendered the formulation applicable t o both prismatic and revolute joints. The versatility of the approach is demonstrated through its implementation to formulate forward kinema tic problems of manipulators with revolute and prismatic joints. Moreo ver, the proposed flexibility matrix is used in the development of a d ynamic model for a compliant spherical robotic manipulator. This task has a dual purpose. First, it demonstrates how the flexibility matrix can be implemented in a systematic approach for deriving the equations of motion of an open-kinematic chain that account for the axial geome tric shortening, the torsional vibration, and the in-plane and out-of- plane transverse deformations of the compliant member. Second, the inc lusion of the torsional vibration in the equations of motion serves to broaden the scope of previous research work done on modelling open-ki nematic chains. The formulation can now address dynamic problems that are not limited to the positioning but are also concerned with the ori entation of rigid body payloads as they are being manipulated by robot ic manipulators. The digital simulation results exhibit the interactio n between the torsional vibration and the rigid body motion of the arm . Furthermore, they demonstrate a strong coupling effect between the t orsional vibration and the transverse deformations of the arm whenever the payload is not grasped at its mass center by the gripper. (C) 199 8 Academic Press.