A fish-type robot driven by snap-through buckling with flexible body

Author(s):  
Tatsuya ITAGAKI ◽  
Daisuke NAKANISHI
Keyword(s):  
2018 ◽  
Vol 108 (10) ◽  
pp. 703-707
Author(s):  
D. Kupzik ◽  
S. Coutandin ◽  
J. Fleischer

Die steigende Variantenvielfalt im Automobilbau durch neue Modelle und elektrische Derivate motiviert ein Umdenken im Karosserierohbau. In „SmartBodySynergy“ (SBS) wird ein flexibler Karosserierohbau in Werkstattfertigung entwickelt. Für dessen Umsetzung sind flexible Fügezellen notwendig. In diesem Artikel wird der Einsatz einer vorrichtungsfreien, kamerageregelten Bauteilpositionierung für den Einsatz in varianten- sowie vorgangsflexiblen Fügezellen untersucht und eine Demonstratorzelle vorgestellt.   The increasing diversity of variants in the automotive industry through new models and electrical derivatives motivates a rethinking of body shop construction. In „SmartBodySynergy“ (SBS), a flexible body shop is being developed in workshop production. For its implementation, flexible joining cells are necessary. This article examines the use of device-free, camera-controlled component positioning for use in variant- and process-flexible joining cells and introduces a demonstrator cell.


2020 ◽  
Vol 2020 (0) ◽  
pp. 513
Author(s):  
Masato TAKEUCHI ◽  
Kensuke HARA ◽  
Hiroshi YAMAURA

Author(s):  
Martin M. Tong

Numerical solution of the dynamics equations of a flexible multibody system as represented by Hamilton’s canonical equations requires that its generalized velocities q˙ be solved from the generalized momenta p. The relation between them is p = J(q)q˙, where J is the system mass matrix and q is the generalized coordinates. This paper presents the dynamics equations for a generic flexible multibody system as represented by p˙ and gives emphasis to a systematic way of constructing the matrix J for solving q˙. The mass matrix is shown to be separable into four submatrices Jrr, Jrf, Jfr and Jff relating the joint momenta and flexible body mementa to the joint coordinate rates and the flexible body deformation coordinate rates. Explicit formulas are given for these submatrices. The equations of motion presented here lend insight to the structure of the flexible multibody dynamics equations. They are also a versatile alternative to the acceleration-based dynamics equations for modeling mechanical systems.


Wind Energy ◽  
10.1002/we.66 ◽  
2002 ◽  
Vol 5 (4) ◽  
pp. 281-300 ◽  
Author(s):  
Donghoon Lee ◽  
Dewey H. Hodges ◽  
Mayuresh J. Patil

2005 ◽  
Vol 38 (1) ◽  
pp. 265-270
Author(s):  
Hiromi Mochiyama ◽  
Hideo Fujimoto

2017 ◽  
Vol 2017 ◽  
pp. 1-18 ◽  
Author(s):  
Dejian Meng ◽  
Lijun Zhang ◽  
Jie Xu ◽  
Zhuoping Yu

To improve the understanding of brake creep groan, both experimental and numerical studies are conducted in this paper. Based on a vehicle road test under the condition of downhill, complicated stick-slip type motion of caliper and its correlation with the interior noise were analyzed. In order to duplicate these brake creep groan phenomena, a transient dynamic model including brake corner and subsystems was established using finite element method. In the model, brake components were considered to be flexible body, and the subsystems including driveline, suspension, tire, and vehicle body were considered to be rigid body. Simulation and experimental results of caliper vibration in time and frequency domains were compared. It was demonstrated that the new model is effective for the prediction and analysis of brake creep groan, and it has higher accuracy compared to the previous model without the subsystems. It is also found that the lining and caliper not only have stick-slip motion in each coordinate direction but also have translational and torsional movements in plane, which relate to the microscopic sticking and slipping, friction coefficient, and forces, as well as the contact status at the friction interface.


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