A passive vibration absorber for reducing the motion of a planar pendulum i
s developed. The system is excited by the horizontal motion of the support.
The design transforms the original one-degree-of-freedom pendulum into a d
ouble pendulum by adding a small secondary pendulating sacrificial mass bet
ween the main system and the base excitation point and two pretensioned spr
ings that generate negative restoring moments (i.e., of opposite sign to th
at of the gravity-induced restoring moments). Optimal conditions for enhanc
ing the transfer of energy from the main (lower) to the secondary (upper) p
endulum are sought. The damping is assumed to be of a linear viscous-type.
Due to the action of the springs, the transfer function between the pendula
tion angle of the main system and the disturbance, in the undamped lineariz
ed case, can be reduced to zero for any excitation frequency. This is accom
plished by requiring that the two spring stiffnesses satisfy an algebraic t
uning relation. Due to the inherent inertial coupling, the two normal coord
inates are coupled through off-diagonal terms in the damping matrix. Hence,
the vibration absorber acts to block the transfer of disturbance energy to
the main system while enhancing the transfer of energy due to initial cond
itions from the main pendulum to the secondary pendulum. The absorber desig
n is based on a frequency-domain approach borrowed from linear theory There
fore, to corroborate the effectiveness of the absorber in the nonlinear ope
rating regime (for higher excitation levels), representative responses to i
nitial conditions and frequency-response curves are computed by applying a
path-following algorithm to the full nonlinear governing equations. The ove
rall effect of the design is somehow a "linearization" of the system behavi
or with increased damping properties. In fact, the proposed absorber reduce
s the response of the system by more than 30 decibels near resonance, exhib
its good attenuation characteristics in a broad range of frequencies away f
rom resonance, and remarkably improves the initial-condition response.