where a is the apex half-angle of the pyramidal indenter, P is the indenting load in kgf and d is the indentation diagonal in mm. The diagonal, d, is measured by means of an optical microscope after unloading the indenter, while the apex half-angle of the indentation, a, is assumed to be constant at all applied loads and equal to the apex half-angle of the indenter, i.e., half of the angle between opposite triangular faces of the indenter (standard a 688). It is well established that in most materials the microhardness measured by means of indentations decreases with increasing indenting load down to a constant value, which coincides with the macrohardness of the material [1]. This phenomenon is called indentation size effect (ISE) and has been observed in many materials, including tungsten carbide (WC) single crystals [2]. This work aimed at assessing the role of elastic relaxation in the observed ISE. For this purpose, a (0 0 0 1) face of a WC crystal was indented at 25, 50, 100, 200 and 500 3 10y3 kg and, after unloading the indenter, the depth and diagonal lengths of the indentations were measured by atomic force microscopy (AFM). The results were compared with the depth and diagonal of the indentations before unloading, which were calculated from the geometry of the indenter. The indenter was a standard Vickers indenter, i.e., a square pyramid of apex half-angle equal to 688. For the calculation of the size of the indentation before unloading, it was assumed that the intrinsic hardness of the WC (0 0 0 1) surfaces was 2000 kgf mmy2, i.e., the macrohardness measured at loads of 1 kg or higher [3]. Fig. 1 shows the percentage change in the depth and the diagonal length of the indentations before and after unloading each of the ®ve indenting loads, as well as the percentage change in Vickers microhardness, relative to the known macrohardness. The percentage change decreases in all cases with increasing indenting load. The microhardness tends to the macrohardness value, and the percentage change in diagonal length tends to zero, but the change in depth tends to approximately 30%. The half-angle â between two opposite edges of the indentation, which, before unloading, is related to the apex angle a by the equation tan â 2 p tan a (2)