Time efficient stiffness model computation for a parallel haptic mechanism via the virtual joint method

2020 ◽  
Vol 143 ◽  
pp. 103614 ◽  
Author(s):  
İbrahimcan Görgülü ◽  
Giuseppe Carbone ◽  
Mehmet İsmet Can Dede
2021 ◽  
pp. 109963622199386
Author(s):  
Tianshu Wang ◽  
Licheng Guo

In this paper, a shear stiffness model for corrugated-core sandwich structures is proposed. The bonding area is discussed independently. The core is thought to be hinged on the skins with torsional stiffness. The analytical model was verified by FEM solution. Compared with the previous studies, the new model can predict the valley point of the shear stiffness at which the relationship between the shear stiffness and the angle of the core changes from negative correlation to positive correlation. The valley point increases when the core becomes stronger. For the structure with a angle of the core smaller than counterpart for the valley point, the existing analytical formulations may significantly underestimate the shear stiffness of the structure with strong skins. The results obtained by some previous models may be only 10 persent of that of the present model, which is supported by the FEM model.


1994 ◽  
Vol 60 (575) ◽  
pp. 2331-2337
Author(s):  
Nobuyuki Iwatsuki ◽  
Iwao Hayashi ◽  
Kazuharu Morishige

2001 ◽  
Vol 2 (4) ◽  
pp. 34-38 ◽  
Author(s):  
Duck-Jung Lee ◽  
Yun-Hi Lee ◽  
Gwon-Jin Moon ◽  
Jun-Dong Kim ◽  
Won-Do Choi ◽  
...  

1995 ◽  
Vol 48 (11S) ◽  
pp. S61-S67 ◽  
Author(s):  
Carlos E. S. Cesnik ◽  
Dewey H. Hodges

An asymptotically exact methodology, based on geometrically nonlinear, three-dimensional elasticity, is presented for cross-sectional analysis of initially curved and twisted, nonhomogeneous, anisotropic beams. Through accounting for all possible deformation in the three-dimensional representation, the analysis correctly accounts for the complex elastic coupling phenomena in anisotropic beams associated with shear deformation. The analysis is subject only to the restrictions that the strain is small relative to unity and that the maximum dimension of the cross section is small relative to the wave length of the deformation and to the minimum radius of curvature and/or twist. The resulting cross-sectional elastic constants exhibit second-order dependence on the initial curvature and twist. As is well known, the associated geometrically-exact, one-dimensional equilibrium and kinematical equations also depend on initial twist and curvature. The corrections to the stiffness model derived herein are also necessary in general for proper representation of initially curved and twisted beams.


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