The wedge test, as used for the evaluation of adhesive fracture energy, is usually considered to be a 2D geometry: its simple analysis implies independence of the width of the adhesive joint, b. Recent work has shown this to be an oversimplification, at least in some circumstances, with (hypothesised) anticlastic bending giving rise to curvature of the crack front. As a result, crack front length, a, varies across the joint width leading to ambiguity in the interpretation of results to obtain fracture energy, G c . This contribution constitutes a more detailed analysis of the geometry of the wedge test (in the particular case of one bending and one rigid substrate), treating the bent member as a plate, rather than as a simple beam. The Kirchhoff-Love plate theory is applied and solved by a perturbation method. Secondary curvature of the beam in the direction normal to the principal curvature results directly from the treatment, and this, in turn, leads to a concave crack front, corroborating the above-mentioned experimental observation.