A B S T R A C T A sickle-shaped surface crack, also called crescent-moon (or crescent) crack, is assumed to exist at the root of a circular-arc circumferential notch in a round bar under tension and bending. For different notch sizes (i.e. different values of the stress concentration factor), the stress intensity factor along the crack front is computed through a three-dimensional finite-element analysis. The effect of the stress concentration factor on the stress intensity factor values is examined for several crack configurations. Finally, the surface crack growth under cyclic loading is analysed through a numerical procedure that employs the stress intensity factor values obtained. Some results of the present study are compared with those by other authors. a = crack depth for point A on the flaw front a el , b el = semi-axes of the ellipse c = notch depth D = bar diameter in the reduced cross-section S-S D 0 = bar diameter in an unnotched cross section F = tension loading K I,F , K * I,F = stress-intensity factor (SIF) and dimensionless SIF, respectively, for tension K I,MX , K * I,MX = stress-intensity factor (SIF) and dimensionless SIF, respectively, for bending M X K t,F , K t,MX = stress-concentration factor (SCF) for tension (F) and bending (M X ), respectively M X = bending loading about the X axis SCF = stress-concentration factor SIF = stress-intensity factor α = a el /b el = aspect ratio of the elliptical-arc crack front δ = c/D 0 = relative notch depth σ F = nominal tensile stress (referred to the reduced cross section) σ MX = nominal maximum bending stress (referred to the reduced cross section) ρ, ρ d = ρ/D 0 = notch radius and dimensionless notch radius ξ = a/D = relative crack depth for point A on the flaw front ζ , ζ * = ζ /h = coordinate and normalized coordinate, respectively, of the generic point P along the crack front Correspondence: A. Carpinteri.