We briefly review the results of experimental and theoretical studies of an
elasticity at low frequencies and we discuss the essential features of mode
ls that explain consistently the key aspects of this behaviour. In our orig
inal paper on this topic we reported that damping in a compound pendulum at
frequencies in the range 10(-3)-10(-2) Hz was consistent with an imaginary
component of Young's modulus for the Cu-Be suspension that was independent
of frequency. Damping with this characteristic frequency dependence can al
so be described in terms of viscous damping whose magnitude varies as the i
nverse of frequency. With the hindsight provided by our further work we now
realize that stick-slip processes can give rise to such losses, not only i
n the suspensions but also in the structures and clamping mechanism of the
suspensions of long-period pendulums.