A contact problem is considered in which an elastic half-plane is pressed a
gainst a rigid fractally rough surface, whose profile is defined by a Weier
strass series. It is shown that no applied mean pressure is sufficiently la
rge to ensure full contact and indeed there are not even any contact areas
of finite dimension-the contact area consists of a set of fractal character
for all values of the geometric and loading parameters.
A solution for the partial contact of a sinusoidal surface is used to devel
op a relation between the contact pressure distribution at scale n-1 and th
at at scale n. Recursive numerical integration of this relation yields the
contact area as a function of scale. An analytical solution to the same pro
blem appropriate at large n is constructed following a technique due to Arc
hard. This is found to give a very good approximation to the numerical resu
lts even at small n, except for cases where the dimensionless applied load
is large.
The contact area is found to decrease continuously with n, tending to a pow
er-law behaviour at large n which corresponds to a limiting fractal dimensi
on of (2 - D), where D is the fractal dimension of the surface profile. How
ever, it is not a 'simple' fractal, in the sense that it deviates from the
power-law form at low n, at which there is also a dependence on the applied
load. Contact segment lengths become smaller at small scales, but an appro
priately normalized size distribution tends to a limiting function at large
n.