A method is proposed to study the stress concentration around a shallow spheroidal crack in an infinite elastic body. The stress concentration is due to the diffraction of a low-frequency plane longitudinal wave by the crack. The direction of wave propagation is established in which the combined concentration of mode I and mode II stresses is maximum Keywords: infinite elastic body, shallow spheroidal crack, plane longitudinal harmonic wave, dynamical stress intensity factorBecause of the spatial asymmetry of external forces, three-dimensional defects such as cracks are in most cases of complex topological structure. Both the varying periphery of the crack and the curvature of its surface were adequately accounted for in static problem statements [1,6,7]. Under a dynamic load generating elastic waves in a certain direction, the level of stress concentration around such cracks is determined by the correlation of the geometries of the defect and the wave diffracted by it. The majority of studies in this area address the dynamic behavior of flat cracks with different outlines [3,5,17,19,20]. A few publications are concerned with nonflat cracks [2,9,11]; those of these publications that deal with three-dimensional problem statements [11] analyze only a wave field far from the defect, which gives a little information on brittle fracture.The present paper examines the three-dimensional opening displacement of a shallow spheroidal crack and mixed-mode stress intensity factors at its boundary, which are due to a plane harmonic wave incident on the crack at an arbitrary angle. Note that a similar crack under harmonic pressure on its surface was studied earlier in [8].