An analysis is presented of the impact of a solid, elastic ball on an
elastic, semi-infinite solid covered by a thin layer of lubricant. The
ball is decelerated by very high hydrodynamic pressures of GPa propor
tions, which also create substantial elastic deformations of the solid
s as the film thicknesses fall to micrometre or sub-micrometre proport
ions. The time of the impact is only slightly longer than that predict
ed by classical Hertzian contact analysis. The central dimple formed i
n the equivalent elastic ball near a rigid plane maintains a near cons
tant film thickness as the impact proceeds, although the radius of the
conjunction grows and then decays rapidly in this dynamic process. Th
e minimum film thickness occurs in a ring whose rapidly changing radiu
s is closely predicted by Hertzian dry impact analysis. The viscous da
mping plays a modest role in the case considered, while the ball rebou
nds to 95.7% of its original drop height. The pressure-time traces in
the centre, and indeed at most locations in the impact zone, exhibit a
remarkable second pressure peak, or spike, to yield a profile very si
milar to the familiar pressure-distance trace from steady state, entra
ining elastohydrodynamic lubrication problems. The findings thus confi
rm the experimental observations of such pressure spikes reported in 1
985 by Safa and Gohar (Proc. 12th Leeds-Lyon Symp. Tribol, 1985). The
new solution procedure outlined in the paper is expected to be useful
in analysing bouncing ball arrangements, used primarily in Sweden, for
theological studies of oils.