“…The obstacle itself may be considered to be moving smoothly, and an important example of an impact oscillator, described in [19], is that of a particle moving under gravity and impacting with a sinusoidally moving table. There is now a comprehensive theory describing the behaviour of these systems, in which we see both periodic and chaotic motions arising, and changing at both smooth bifurcations (saddle-node, period-doubling etc) and non-smooth events such as grazing bifurcations [26,27] and chattering sequences [8].…”