For a block with a hole of size R with a force/unit length of F, the stress tex2html_wrap140 where W is the width. The stress near the hole is something like: tex2html_wrap141

For a hole of length L (very ellipsoidal), with radius of curvature at the ends, R, the energy of the distorted stress region is tex2html_wrap142 . Then tex2html_wrap143 . The minimum R is on the level of the atomic size. This means tex2html_wrap144 . This is too low. creation of cracks involves surface tension. propagation condition is tex2html_wrap145 . Then tex2html_wrap146 = griffith crack length. tex2html_wrap147 . This means tex2html_wrap148 . Surface is actually jagged, increasing the real crack length. tex2html_wrap149 =work of fracture which is typically, tex2html_wrap150 . Then tex2html_wrap151 sometimes, but the crack does not propagate. propagation condition: tex2html_wrap152 .

There should really be a kinetic term, because the cracks can propagate at the speed of sound.

tex2html_wrap157 for tex2html_wrap158 you get the griffith crack length.

tex2html_wrap159 . Crack can accelerate over time. Stresses tend to be perpendicular to the crack. Instability in crack growth is onset at tex2html_wrap160 .




source psfile jl@crush.caltech.edu index