AbstractThe commonly used fracture criteria-maximum KI, zero KII, maximum hoop-stress, and maximum energy-release rate-predict similar fracture paths in isotropic materials, but not in anisotropic materials. In the general anisotropic case, the fracture path depends on the material-symmetry properties, the nature of the applied loads, and the overall geometry of the specimen. In addition, anisotropy in the material's resistance to fracturing plays a key role in defining crack initiation and its propagation path. Experiments are performed on notched specimens made from sapphire, a microscopically homogeneous and brittle single-crystal solid. The force required for fracture initiation is measured. The experimental measurements/observations are compared with the numerical results of the FEM simulations. A stress-based fracture parameter,
$$A = \sqrt {2\pi R_0 \sigma _N } /\sqrt {\gamma _N E_N } $$
is shown to be a good measure of the fracture criterion, where σ and E, respectively, are the tensile stress and Young's modulus in the direction normal to the cleavage plane, with surface energy γ , and R is a characteristic length, e.g., the notch radius. This parameter takes into account the effects of the surface energy of the corresponding cleavage plane, as well as the strength of the atomic bonds in the direction normal to the cleavage plane. More than two-thirds of the notched specimens fractured at the point and along a cleavage plane where A is maximum. The measurements of the applied force made it possible to quantitatively obtain a critical value for parameter A. Finally, experiments show that for the notched sapphire specimens the weakest family of cleavage planes,
$$\{ \bar 1012\} {\text{ and \{ }}10\bar 10{\text{\} }} $$
, are the fracture planes, although a few specimens fractured along non-cleavage planes.
[1]
J. B. Wachtman,et al.
Elastic Constants of Synthetic Single Crystal Corundum at Room Temperature
,
1960,
Journal of research of the National Bureau of Standards. Section A, Physics and chemistry.
[2]
Stephen W. Tsai,et al.
A General Theory of Strength for Anisotropic Materials
,
1971
.
[3]
Carl T. Herakovich,et al.
A Normal Stress Criterion for Crack Extension Direction in Orthotropic Composite Materials
,
1985
.
[4]
Takashi Miyata,et al.
The condition of fatigue crack growth in mixed mode condition
,
1975
.
[5]
G. Sih,et al.
A SPECIAL THEORY OF CRACK PROPAGATION METHODS OF ANALYSIS AND SOLUTION OF CRACK PROBLEMS
,
1973
.
[6]
F. Erdogan,et al.
On the Crack Extension in Plates Under Plane Loading and Transverse Shear
,
1963
.
[7]
S. Nemat-Nasser,et al.
Energy-release rate and crack kinking in anisotropic brittle solids
,
1996
.
[8]
S. Nemat-Nasser,et al.
Experimental and computational study of fracturing in an anisotropic brittle solid
,
1998
.
[9]
J. Gilman,et al.
Direct Measurements of the Surface Energies of Crystals
,
1960
.
[10]
R. P. Ingel,et al.
Elastic Anisotropy in Zirconia Single Crystals
,
1988
.
[11]
S. Nemat-Nasser,et al.
Hoop stress intensity factor and crack-kinking in anisotropic brittle solids
,
1996
.
[12]
S. Nemat-Nasser,et al.
Toughening by partial or full bridging of cracks in ceramics and fiber reinforced composites
,
1987
.
[13]
S. Wiederhorn.
Fracture of Sapphire
,
1969
.
[14]
Yoshiaki Goto,et al.
Branched cracks in anisotropic elastic solids
,
1989
.