Contact problems are central to Solid Mechanics, because contact is the pri
ncipal method of applying loads to a deformable body and the resulting stre
ss concentration is often the most critical point in the body. Contact is c
haracterized by unilateral inequalities, describing the physical impossibil
ity of tensile contact tractions (except under special circumstances) and o
f material interpenetration. Additional inequalities and/or non-linearities
are introduced when friction laws are taken into account. These complex bo
undary conditions can lead to problems with existence and uniqueness of qua
si-static solution and to lack of convergence of numerical algorithms, In f
rictional problems, there can also be lack of stability, leading to stick-s
lip motion and frictional vibrations.
If the material is non-linear, the solution of contact problems is greatly
complicated, but recent work has shown that indentation of a power-law mate
rial by a power law punch is self-similar, even in the presence of friction
, so that the complete history of loading in such cases can be described by
the (usually numerical) solution of a single problem.
Real contacting surfaces are rough, leading to the concentration of contact
in a cluster of microscopic actual contact areas. This affects the conduct
ion of heat and electricity across the interface as well as the mechanical
contact process. Adequate description of such systems requires a random pro
cess or statistical treatment and recent results suggest that surfaces poss
ess fractal properties that can be used to obtain a more efficient mathemat
ical characterization.
Contact problems are very sensitive to minor profile changes in the contact
ing bodies and hence are also affected by thermoelastic distortion. Importa
nt applications include cases where non-uniform temperatures are associated
with frictional heating or the conduction of heat across a non-uniform int
erface. The resulting coupled thermomechanical problem can be unstable, lea
ding to a rich range of physical phenomena.
Other recent developments are also briefly surveyed, including examples of
anisotropic materials, elastodynamic problems and fretting fatigue. (C) 199
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