Kinematics Constraint Modeling for Flexible Robots based on Deep Learning1

Author(s):  
Olatunji Mumini Omisore ◽  
Lei Wang
1991 ◽  
Vol 26 (8) ◽  
pp. 27-36
Author(s):  
Richard C. Waters

2020 ◽  
pp. 421-454
Author(s):  
K. Desoyer ◽  
P. Lugner ◽  
I. Troch ◽  
P. Kopacek

2003 ◽  
Vol 56 (6) ◽  
pp. 553-613 ◽  
Author(s):  
Tamer M Wasfy ◽  
Ahmed K Noor

The status and some recent developments in computational modeling of flexible multibody systems are summarized. Discussion focuses on a number of aspects of flexible multibody dynamics including: modeling of the flexible components, constraint modeling, solution techniques, control strategies, coupled problems, design, and experimental studies. The characteristics of the three types of reference frames used in modeling flexible multibody systems, namely, floating frame, corotational frame, and inertial frame, are compared. Future directions of research are identified. These include new applications such as micro- and nano-mechanical systems; techniques and strategies for increasing the fidelity and computational efficiency of the models; and tools that can improve the design process of flexible multibody systems. This review article cites 877 references.


Author(s):  
Alessandro De Luca
Keyword(s):  

2006 ◽  
Vol 11 (6) ◽  
pp. 690-698 ◽  
Author(s):  
Shuzhi Sam Ge ◽  
Keng Peng Tee ◽  
Ivan E. Vahhi ◽  
Francis E. H. Tay

Author(s):  
Hidenori Murakami ◽  
Oscar Rios ◽  
Takeyuki Ono

For actuator design and motion simulations of slender flexible robots, planar C1-beam elements are developed for Reissner’s large deformation, shear-deformable, curbed-beam model. Internal actuation is mechanically modeled by a rate-form of beam constitutive relation, where actuation curvature is prescribed at each time. Geometrically, a curbed beam is modeled as a frame bundle, whereby at each point on beam’s curve of centroids a moving orthonormal frame is attached to a cross section. After a finite element discretization, a curve of centroids is modeled as a C1-curve, employing cubic shape functions for both planar coordinates with an arc-parameter. The cubic shape functions have already been utilized in linear Euler-Bernoulli beams for the interpolation of transverse displacement. To define the rotation angle of each cross section or the attitude of the moving frame, quadratic shape functions are used introducing a middle node, resulting in three angular nodal displacements. As a result, each beam element has total eleven nodal coordinates. The implementation of a nonlinear finite element code is facilitated by the principle of virtual work, which yields Reissner’s large deformation curbed beam model as the Euler-Lagrange equations. For time integration, the Newmark method is utilized. Finally, as applications of the code, a few inchworm motions induced by different actuation curvature fields are presented.


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