The measurement of ultrasonic reflection has been used to study the contact
between rough surfaces. An incomplete interface will reflect some proporti
on of an incident wave; this proportion is known as the reflection coeffici
ent. If the wavelength is large compared with the width of the gaps in the
plane of the interface then the reflection mechanism can be modeled by cons
idering the interface as a spring. The proportion of the incident wave refl
ected (reflection coefficient) is then a function of the stiffness of the i
nterface and the frequency of the ultrasonic wave. The sensitivity of the u
ltrasonic technique has been quantified using a simple model, from which th
e stiffness of individual gaps and contacts are calculated and their effect
on the ultrasonically measured stiffness predicted. The reflection of ultr
asound at a static interface between a rough, nominally flat aluminum plate
and a rough, nominally flat hardened steel punch has been investigated. Pl
astic flow on first loading was evident, while repeated loading was largely
elastic. However, subsequent cycles indicate a small amount of further pla
sticity and contact irreversibility. The effect of surface roughness on the
resultant contact has also been investigated. A simple plastic contact mod
el is described which allows prediction of the average size of the asperity
contacts and their number. This model shows that the average size of the c
ontracts remains constant over most of the loading whereas the number of co
ntacts increases almost linearly. The contact stiffness has also been model
ed with two well known elastic rough surface contact models. These models p
redicted a lower interface stiffness than was observed in the experiments.
However they provide a useful way of interpreting the ultrasonically measur
ed interface stiffness data.