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Once we realize that stress concentrators exist, the next step is to consider how they may exist in a material and how these will influence fracture. A. A. Griffith did some of the pioneering work in this area, alongside others. A key thing to recognize is that all materials have flaws and that the most severe flaw will govern failure if the maximum stress at the crack tip exceeds the yield strength of the material. The next point is that stress on a material causes two considerations. First, lattice strain occurs raising the energy of the system. This could be relieved by crack growth since it would return lattice to normal as crack separates the strained material. Second, the crack propagation will create a surface with some associated energy. Whether a crack propagates depends on the balance of strain energy release vs surface energy formation. We can observe a critical stress intensity factor that is equal to a dimensionless shape parameter, Y, the applied stress, and the square root of pi times the half-crack length, a.