scholarly journals First-order rotation solution of an oblate rigid body under the torque of a perturber in circular orbit

2010 ◽  
Vol 519 ◽  
pp. A1 ◽  
Author(s):  
M. Lara ◽  
T. Fukushima ◽  
S. Ferrer
Author(s):  
Martin B. Hamper ◽  
Cheng Wei ◽  
Ahmed A. Shabana

In the analysis of multibody system (MBS) dynamics, contact between two arbitrary rigid bodies is a fundamental feature in a variety of models. Many procedures have been proposed to solve the rigid body contact problem, most of which belong to one of the two categories: offline and online contact search methods. This investigation will focus on the development of a contact surface model for the rigid body contact problem in the case where an online three-dimensional nonconformal contact evaluation procedure, such as the elastic contact formulation—algebraic equations (ECF-A), is used. It is shown that the contact surface must have continuity in the second-order spatial derivatives when used in conjunction with ECF-A. Many of the existing surface models rely on direct linear interpolation of profile curves, which leads to first-order spatial derivative discontinuities. This, in turn, leads to erroneous spikes in the prediction of contact forces. To this end, an absolute nodal coordinate formulation (ANCF) thin plate surface model is developed in order to ensure second-order spatial derivative continuity to satisfy the requirements of the contact formulation used. A simple example of a railroad vehicle negotiating a turnout, which includes a variable cross-section rail, is tested for the cases of the new ANCF thin plate element surface, an existing ANCF thin plate element surface with first-order spatial derivative continuity, and the direct linear profile interpolation method. A comparison of the numerical results reveals the benefits of using the new ANCF surface geometry developed in this investigation.


2015 ◽  
Vol 8 (2) ◽  
Author(s):  
Sangamesh R. Deepak ◽  
Amrith N. Hansoge ◽  
G. K. Ananthasuresh

There are analytical methods in the literature where a zero-free-length spring-loaded linkage is perfectly statically balanced by addition of more zero-free-length springs. This paper provides a general framework to extend these methods to flexure-based compliant mechanisms through (i) the well know small-length flexure model and (ii) approximation between torsional springs and zero-free-length springs. We use first-order truncated Taylor's series for the approximation between the torsional springs and zero-free-length springs so that the entire framework remains analytical, albeit approximate. Three examples are presented and the effectiveness of the framework is studied by means of finite-element analysis and a prototype. As much as 70% reduction in actuation effort is demonstrated. We also present another application of static balancing of a rigid-body linkage by treating a compliant mechanism as the spring load to a rigid-body linkage.


2018 ◽  
Vol 55 (5) ◽  
pp. 1291-1299 ◽  
Author(s):  
Cody Allard ◽  
Hanspeter Schaub ◽  
Scott Piggott

2000 ◽  
Vol 122 (4) ◽  
pp. 669-673 ◽  
Author(s):  
T. Floquet ◽  
W. Perruquetti ◽  
J.-P. Barbot

This paper is devoted to the stabilization of the angular velocity of a rigid body via variable structure based controllers. The system is supposed to have only two control torques and to be subject to external disturbances. A finite time convergence is obtained by switching between a first-order and a second-order sliding mode controllers. [S0022-0434(00)00304-X]


1995 ◽  
Vol 11 (4) ◽  
pp. 545-557 ◽  
Author(s):  
J.C. Trinkle ◽  
A.O. Farahat ◽  
P.F. Stiller
Keyword(s):  

1970 ◽  
Vol 26 (2) ◽  
pp. 260-262 ◽  
Author(s):  
G. S. Pawley ◽  
B. T. M. Willis

The analysis in part I is generalized to any crystal containing rigid molecules which undergo anisotropic translational and librational motion about a site fixed by symmetry. The treatment is correct to terms in (ui 2)2 and (ωi 2)2, where (ui 2) is the mean-square translational displacement of the molecule along the ith axis and (ωi 2) is the mean-square angular libration about the same axis. The first-order treatment to terms in (ui 2) and (ωi 2) is shown to be equivalent to the rigid-body theory in current use.


1997 ◽  
Vol 92 (3) ◽  
pp. 481-489
Author(s):  
Z. Niedzielska ◽  
P. Wąż

1996 ◽  
Vol 63 (1) ◽  
pp. 149-155 ◽  
Author(s):  
P. Tsiotras ◽  
J. M. Longuski

The problem of the time evolution of the angular velocity of a spinning rigid body, subject to torques about three axes, is considered. An analytic solution is derived that remains valid when no symmetry assumption can be made. The solution is expressed as a first-order correction to a previous solution, which required a symmetry or near-symmetry assumption. Another advantage of the new solution (over the former) is that it remains valid for large initial conditions of the transverse angular velocities.


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