It is by now well established that loading conditions
with sufficiently large triaxialities can induce the sudden appearance of
internal cavities within elastomeric (and other soft) solids. The occurrence of
such instabilities, commonly referred to as cavitation, can be attributed to
the growth of pre-existing defects into finite sizes.
In this talk, I will present a new theory to study the
phenomenon of cavitation in soft solids that, contrary to existing approaches,
simultaneously: (i) allows to consider general 3D loading
conditions with arbitrary triaxiality, (ii)
applies to large (including compressible and anisotropic) classes of
nonlinear elastic solids, and
(iii) incorporates direct information on the initial
shape, spatial distribution, and mechanical properties of the underlying
defects at which cavitation can initiate. The basic idea is to first cast
cavitation in elastomeric solids as the homogenization problem of nonlinear
elastic materials containing random distributions of zero-volume cavities, or
defects. Then, by means of a novel iterated homogenization procedure, exact
solutions are constructed for such a problem. These include solutions for the
change in size of the underlying cavities as a function of the applied loading
conditions, from which the onset of cavitation - corresponding to the event
when the initially infinitesimal cavities suddenly grow into finite sizes - can
be readily determined. In spite of the generality of the proposed approach, the
relevant calculations amount to solving tractable Hamilton-Jacobi equations, in
which the initial size of the cavities plays the role of "time" and
the applied load plays the role of "space".
An application of the theory to the case of Ne-Hookean
solids containing a random isotropic distribution of vacuous defects will be
presented.