There are two types of distinct periodic dynamic waves in the history of th
e wheel/rail contact force. The first is caused by the variation in overall
track stiffness owing to the effect of tie spacing. The second is caused b
y the travelling motion of the wheel and the oscillations of discrete suppo
rts, In the present train speed range these dynamic forces are usually less
than 5 per cent of the static load, except that the coupled wheel/track re
sonant frequencies are excited at some speeds. The resonant forces due to d
iscrete supports may be larger than 5 per cent of the static load in some c
ases. The magnitude of the resonant force mainly depends on the unsprung ma
ss, tie spacing, vehicle primary and track ballast damping, rail stiffness
and the stiffness on each support.