“…In the case of a transverse planar flaw located in the ( x , y ) plane, the spatial variable x along the thickness of the flaw disappears, and the flaw is represented by a current surface dipole density, referred to as p ( y , z ), which is a scalar quantity depending on two spatial variables corresponding to the dimensions of the surface of the ideal flaw. The surface dipole density is solution of an integral equation on the surface of the crack, which involves an hypersingular kernel when it is evaluated in the spatial domain (Beltrame and Burais, 2002a, b). In an alternative way, the kernel can be evaluated in the spectral domain (Pávó and Miya, 1994), and the use of a global approximation of p ( y , z ) (Pávó and Lesselier, 2006) may overcome some numerical difficulties coming from specific boundary conditions to be satisfied by p ( y , z ) (Bowler et al , 1997).…”