๐”– Bobbio Scriptorium
โœฆ   LIBER   โœฆ

The stability and response of a flexible rod in a quick return mechanism

โœ Scribed by D.G. Beale; R.A. Scott


Publisher
Elsevier Science
Year
1990
Tongue
English
Weight
836 KB
Volume
141
Category
Article
ISSN
0022-460X

No coin nor oath required. For personal study only.


๐Ÿ“œ SIMILAR VOLUMES


The Stability and Response of a Flexible
โœ D.G. Beale; R.A. Scott ๐Ÿ“‚ Article ๐Ÿ“… 1993 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 377 KB

The response and stability of a flexible rod, rigid crank quick return mechanism is investigated without a small crank restriction. A Galerkin's approach was found to be too computationally intensive, due to the moving boundary and complex mode shapes, and thus unsuitable for monodromy based paramet

DYNAMIC ANALYSIS OF THE FLEXIBLE ROD OF
โœ R.-F. Fung; F.-Y. Lee ๐Ÿ“‚ Article ๐Ÿ“… 1997 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 278 KB

The transient amplitude, dynamic stability and steady-state response of a flexible rod of a high-speed quick-return mechanism are investigated in this paper. The crank drives the rod by means of a translating/rotating joint at a constant speed. The flexible rod is divided into two regions. Each regi

Dynamic analyses of a flexible quick-ret
โœ Jih-Lian Ha; Jer-Rong Chang; Rong-Fong Fung ๐Ÿ“‚ Article ๐Ÿ“… 2006 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 547 KB

The finite difference method (FDM) with fixed and variable grids is proposed to approximate the numerical solutions of a flexible quick-return mechanism. In the dynamic analysis and simulation, the flexible rod is divided into two regions. Each region with time-dependent length is modeled by Euler-b

VIBRATION SUPPRESSION AND MOTION CONTROL
โœ Rong-Fong Fung; Ken-Wang Chen ๐Ÿ“‚ Article ๐Ÿ“… 1998 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 387 KB

This paper studies both speed and tracking controls of a non-linear flexible quick-return mechanism driven by a permanent magnet (PM) synchronous servo motor. A flexible rod of the mechanism is divided into two regions. Each region has a time-dependent length and is modelled by the Timoshenko beam t