D. Filipovic et D. Schroder, Vibration absorption with linear active resonators: Continuous and discrete time design and analysis, J VIB CONTR, 5(5), 1999, pp. 685-708
The concept of the linear active resonator (LAR) as a vibration absorber is
presented. It is formed of a classical passive absorber with a simple dyna
mic linear feedback. The LAR is, on one hand, a well-known passive absorber
but has, on the other hand, an additional actuator that produces a force (
lateral system) or a torque (rotational system). This additional actuator i
s controlled by a feedback signal that is processed in a linear compensator
and the reference value for the actuator is produced. The parameters in th
e compensator are set to produce a designated resonance frequency in the LA
R, that is, the damping of the passive absorber is "removed." As a result,
the LAR becomes an ideal resonator that theoretically absorbs vibrations fr
om the point of attachment completely The resonant frequency of the LAR is
variable in real time. It is also shown that with this concept the absorber
can have more than one resonant frequency, though it is a single-degree-of
-freedom system. This active absorber does not need information from the pr
imary system that it is attached to; it is autonomous in online operation.
The signal used for the absorber feedback is either the position, velocity
or acceleration of the absorber mass. Depending on the application and conv
enience, this signal can be an absolute one, or a signal relative to the po
int of attachment. The global system characteristics are used only in the o
ff-line analysis, such as for stability and robustness analysis. In this pa
per, the general concept of the LAR is derived in the continuous and the di
screte time domain; the stability analysis of the system with LAR is presen
ted using parameter space analysis.