Tensile cracks (Structure)
Introduction
A stress concentration (also called stress concentrator) is a location within an elastic solid where the local stress is significantly greater than the nominal applied load. An object is stronger when the force is distributed uniformly over its area, such that a reduction in the effective area, for example caused by a crack, leads to an increase in stress near the limit of said defect (compared to the situation in which said defect did not exist). A material can fail by crack propagation when a stress concentration exceeds the limit of the material even though the average stress is below the resistance limit.
The actual fracture resistance of a material is always lower than the theoretical value precisely because most resistant elements contain small cracks or impurities that create a stress concentrator. Fatigue cracks always begin as stress concentrators, so eliminating these defects increases fatigue resistance.
Causes
Geometric discontinuities or lack of smoothness in a geometry act as stress concentrators. Crack ends, sharp corners, holes, and changes in cross section are examples of stress concentrators. High local stresses can produce earlier failure of a resisting element, so engineers design geometries to minimize stress concentration.
Prevention
One measure to prevent the worst types of concentrators, cracks, is to drill a large hole at the end of the crack. This measure may seem counterintuitive, but in fact the internal structure of the compact part of the bones has osteons that can serve this function. The measure works because the radius of curvature of the stress concentrator actually becomes larger, since the tip of a crack is a sharper defect than a hole. Thus, the drilled hole, with its larger diameter, has a lower stress concentration associated with it than the sharp end of the crack.
It is important to systematically verify the existence of stress concentrators associated with cracks. There is a critical length of the crack, such that if this value is exceeded, the crack continues to grow until catastrophic failure occurs. Once the crack exceeds the critical length, no additional stress increase is required to cause the crack to continue growing, so the crack continues to grow until complete failure. Griffith's theory within fracture mechanics serves to explain why there is a critical fracture length.