Boundary kinematic control of a distributed oscillatory system

2007 ◽  
Vol 71 (6) ◽  
pp. 862-868 ◽  
Author(s):  
L.D. Akulenko
Keyword(s):  
Oscillatory System ◽  
Kinematic Control

scholarly journals Kinematic Control of Compliant Serial Manipulators Composed of Dual-Triangles

2021 ◽  
Author(s):  
Wanda Zhao ◽  
Anatol Pashkevich ◽  
Alexandr Klimchik ◽  
Damien Chablat
Keyword(s):  
Serial Manipulators ◽  
Kinematic Control

scholarly journals Kinematic control of extreme jump angles in the red-legged running frog,Kassina maculata

2017 ◽  
Vol 220 (10) ◽  
pp. 1894-1904 ◽  
Author(s):  
Christopher Thomas Richards ◽  
Laura Beatriz Porro ◽  
Amber Jade Collings
Keyword(s):  
Kinematic Control

scholarly journals Intuitive Kinematic Control of a Robot Arm via Human Motion

2014 ◽  
Vol 79 ◽  
pp. 411-416 ◽  
Author(s):  
Hsien-I Lin ◽  
Yu-Cheng Liu ◽  
Yu-Hsiang Lin
Keyword(s):  
Human Motion ◽  
Robot Arm ◽  
Kinematic Control

Preliminary Investigations of Machine Frame Vibration Damping Using Eddy Current Principle

2016 ◽  
Vol 821 ◽  
pp. 288-294 ◽  
Author(s):  
George Juraj Stein ◽  
Peter Tobolka ◽  
Rudolf Chmúrny
Keyword(s):  
Mathematical Model ◽  
Natural Frequency ◽  
Eddy Current ◽  
Asynchronous Motor ◽  
Oscillatory System ◽  
Vibration Damping ◽  
Combined Effects ◽  
Magnetic Forces ◽  
Novel Approach ◽  
Vibration Attenuation

A novel approach to vibration attenuation, based on the eddy current principle, is described. The combined effects of all magnetic forces acting in the oscillatory system attenuate frame vibrations and, concurrently, decrease the damped natural frequency. A mathematical model of the forces balance in the oscillatory system was derived before. Some experimental results from a mock-up machine frame excited by an asynchronous motor are presented.

Closed-Form Expression for the Exact Period of a Nonlinear Oscillator Typified by a Mass Attached to a Stretched Wire

2011 ◽  
Vol 3 (6) ◽  
pp. 689-701
Author(s):  
Malik Mamode
Keyword(s):  
Harmonic Balance ◽  
Nonlinear Oscillator ◽  
Harmonic Balance Method ◽  
Elliptic Functions ◽  
Oscillatory System ◽  
Balance Method ◽  
Closed Form Expression ◽  
Form Expression ◽  
Polynomial Potential ◽  
Exact Analytical Expression

AbstractThe exact analytical expression of the period of a conservative nonlinear oscillator with a non-polynomial potential, is obtained. Such an oscillatory system corresponds to the transverse vibration of a particle attached to the center of a stretched elastic wire. The result is given in terms of elliptic functions and validates the approximate formulae derived from various approximation procedures as the harmonic balance method and the rational harmonic balance method usually implemented for solving such a nonlinear problem.

scholarly journals Birhythmicity, synchronization, and turbulence in an oscillatory system with nonlocal inertial coupling

2005 ◽  
Vol 205 (1-4) ◽  
pp. 154-169 ◽  
Author(s):  
Vanessa Casagrande ◽  
Alexander S. Mikhailov
Keyword(s):  
Oscillatory System ◽  
Inertial Coupling

MULTI–INERT OSCILLATORY MECHANISM

2020 ◽  
Vol 2 ◽  
pp. 19-25
Author(s):  
I.P. POPOV
Keyword(s):  
Kinetic Energy ◽  
Potential Energy ◽  
Oscillation Frequency ◽  
Free Oscillation ◽  
Initial Conditions ◽  
Oscillatory System ◽  
Harmonic Oscillations ◽  
Oscillatory Systems ◽  
Oscillatory Mechanism ◽  
Mutual Conversion

A mechanical oscillatory system with homogeneous elements, namely, with n massive loads (multi– inert oscillator), is considered. The possibility of the appearance of free harmonic oscillations of loads in such a system is shown. Unlike the classical spring pendulum, the oscillations of which are due to the mutual conversion of the kinetic energy of the load into the potential energy of the spring, in a multi–inert oscillator, the oscillations are due to the mutual conversion of only the kinetic energies of the goods. In this case, the acceleration of some loads occurs due to the braking of others. A feature of the multi–inert oscillator is that its free oscillation frequency is not fixed and is determined mainly by the initial conditions. This feature can be very useful for technical applications, for example, for self–neutralization of mechanical reactive (inertial) power in oscillatory systems.

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