Stress intensity factors for penny and halfpenny shaped. Propagation of a pennyshaped hydraulic fracture parallel. The sifs which are exact for a penny shaped crack are based on the well known solution for a point load acting normally to such a crack. Analysis of the data showed that stress intensity factors based on classical halfpenny crack shapes overestimate toughness values and produce an apparent rcurve effect. Introduction to fracture mechanics david roylance department of materials science and engineering massachusetts institute of technology cambridge, ma 029. The sifs which are exact for a penny shaped crack are. The crack length is correlated with the stress intensity factor sif at the crack front and material elastoplastic properties via explicit relationships. Stress intensity factors for a penny shaped crack in a. The throughthickness specimens have a thickness of only three lattice unit cells in the zdirection, so this is only a semi3d system. It is known that a half pennyshaped crack is formed after indentation in some brittle materials chandrasekar and chaudhri, 1993 and in piezoceramics sun and park, 1995. In 4, expressions of this type were evaluated by numerically computing at many discrete values of and applying a numerical integration scheme. Ultrasonic scattering from a crack which emanates from a. The coins featured the head of a nameless miss liberty one of the few females on our. It is noted that the crack front forms a perfect half circle.
Atomistic modeling of pennyshaped and throughthickness. Stress intensity factor of a pennyshaped crack with small. The interface pennyshaped crack reconsidered 169 where 41 42 it can be shown that kw,g has the following property we note that in the present form the size of the contact region, l. Elastodynamic problem for a layered composite with penny. Stress intensity factors 243 where is a function determined by the stress distribution on the crack surface. All specimens have lengths l in x and ydirections of about 600a. On radial crack and halfpenny crack induced by vickers. In this paper we analyze the problem of a pennyshaped hydraulic fracture propagating parallel to the freesurface of an elastic halfspace.
The throughthickness cracks all have a halflength aof about 60a, and the pennyshaped cracks correspondingly have a radius a of approximately 60a. Penny shaped crack in an infinite domain under uniaxial tension. The fracture is driven by an incompressible newtonian fluid injected at a constant rate at the center of the fracture. Based on the stress fields formed upon vickers indentation, the radial crack and halfpenny crack systems are analysed separately using finiteelement analyses. The crack lies in a plane containing the axis of the cylindrical void, also the crack intersects the void at its own axis of symmetry. Crack shape effects in fracture toughness measurements. Uniform uniaxial stress edit if the crack is located centrally in a finite plate of width 2 b \displaystyle 2b and height 2 h \displaystyle 2h, an approximate relation for the stress intensity factor is 5. At least two types of cracks are produced by a vickers indenter, i. Stress intensity factors at any point on the crack front of penny and halfpenny shaped cracks subjected to stress gradients are presented.
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