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Impact oscillators are a special class of continuous time dynamical
systems which undergo intermittent impact collisions. This class of
oscillator systems have dynamical trajectories in state space which
are piecewise continuous, with discontinuities in the velocities
resulting from the collisions. Even if a system without impact is
linear, and therefore well behaved, the overall dynamics of the system
exhibits a rich variety of behavior because of the nonlinearity
introduced by the impacts.
Impact oscillators can be used to model a variety of systems arising
naturally in many applications. Some of the first impacting oscillators
to be studied were models of various atomic and sub-atomic particle
interactions. In 1949 Fermi [1] proposed a mechanism for the
acceleration of cosmic rays that involved collisions with magnetic
field structures. This mathematically reduces to the study of a particle
moving between two walls, one which is oscillating and the other
stationary,
bouncing elastically off each wall. More recently many engineering systems
like rattling gears [2,3], vibration absorbers
[4], car suspensions [5], impact print hammers
[6], articulated mooring tower [7] and slider-crank
joints [8] have been studied using impact oscillator
models. These systems have motion limiting constraints
occurring naturally in their operation. Repeated impacts, referred to
as vibro-impact response, possibly allied with sliding, is a potent
damage producing mechanism for many types of mechanical devices. They
lead to excessive noise, wear and fatigue.
Impact phenomena are also relevant to the study of biological and
electrical systems, such as studies of
walking [9] and in DC-DC buck converters [10],
respectively. In buck converters, the action of the pulse width modulation
of the supply is very similar to an impacting process.
Investigation of such systems is particularly useful because these
chaotic oscillations can be related to distinct types of dynamic
phenomena and serve as reliable indicators of specific problems
[11]. Furthermore, understanding the dynamics of the system
could help improve the overall system performance by being able to
control the system in some desired regime or by preventing the system
from going into some undesirable regime which would eventually result
in system failure.
In the study of vibro-impact problems, two different approaches
are generally used to model the impact phenomenon. In the first model, it
is assumed that the impacting bodies are elastic with linear or bilinear or
nonlinear stiffness and damping. In the second model, it is assumed that
the impacting bodies are rigid and that the velocity changes instantly,
with the outgoing velocity being a function of the incoming velocity. In
the second approach to modelling the impact phenomena is essentially like
assuming an infinite stiffness coefficient with dissipation and the impacting
process is instantaneous. In our investigations we follow the latter approach
to model impact process. Though, we use the bilinear model of the impact process
to understand the phenomena of hysteresis.
- [1]
-
E. Fermi, Phys. Rev. 75, 1169-1174, (1949).
- [2]
- K. Karagiannis and F. Pfeiffer,
Nonlinear Dynamics 2, 367-387 (1991).
- [3]
- A. Kahraman and R. Singh,
J. Sound Vib. 142, 49-75 (1990).
- [4]
- M. Sharif-Bakhtiar and S. W. Shaw,
J. Sound Vib. 126, 221-235 (1988).
- [5]
- A. Stensson, C. Asplund and L. Karlsson,
Preprint, Lulea University of Technology, Sweden.
- [6]
- P. C. Tung and S. W. Shaw,
J. Vib. Acoust. Stress Reliability Design 110, 193-200 (1988).
- [7]
-
J. M. T. Thompson and H. B. Stewart, Nonlinear Dynamics and Chaos,
(1988) Chichester: Wiley;
- [8]
-
F. Farahanchi and S. W. Shaw, J. Sound Vib., 177
307 (1994),
- [9]
-
T. McGeer, Int. J. of Robotics Res. 9, 62-82 (1990),
- [10]
-
M. diBernardo, E Fossas, G. Olivar and F. Vasca, Applied Nonlinear Mathematics
Report, University of Bristol, 14 (1996),
- [11]
- C. Knudsen, R. Feldberg and H. True,
Philos. Trans. R. Soc. London. A 338, 445-469 (1992).
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