In this paper, the effect of material anisotropy on void nucleation an
d growth in incompressible nonlinearly elastic solids is examined. A b
ifurcation problem is considered for a solid sphere composed of an inc
ompressible homogeneous nonlinearly elastic material which is transver
sely isotropic about the radial direction. Under a uniform radial tens
ile dead-load, a branch of radially symmetric configurations involving
a traction-free internal cavity bifurcates from the undeformed config
uration at sufficiently large loads. Closed form analytic solutions ar
e obtained for a specific material model, which may be viewed as a gen
eralization of the classic neo-Hookean model to anisotropic materials.
In contrast to the situation for a neo-Hookean sphere, bifurcation he
re may occur locally either to the right (supercritical) or to the lef
t (subcritical), depending on the degree of anisotropy. In the latter
case, the cavity has finite radius on first appearance. Such a discont
inuous change in stable equilibrium configurations is reminiscent of t
he snap-through buckling phenomenon of structural mechanics. Such dram
atic cavitational instabilities were previously encountered by Antman
and Negron-Marrero [3] for anisotropic compressible solids and by Horg
an and Pence [17] for composite incompressible spheres.