The study of the microhardness of undoped and doped crystals and the way in which this parameter is connected with the dislocation density is of great interest for transducer applications involving mechanical vibrations [1, 2]. Microhardness gives information about the deformation resistance near the surface, anisotropy in the crystals, evidence for multiphase in the crystals, etc. Tartrates of calcium and strontium crystallize in the orthorhombic system with space group P212121 [3-5] showing ferroelectric properties [6]. Growth of these crystals doped with cobalt, nickel, etc., has drawn considerable interest recently [7, 8]. We carried out microhardness studies on both doped and undoped strontium tartrate tetrahydrate single crystals, using a diamond pyramid indentor. Crystals of strontium tartrate tetrahydrate were grown in silica gel medium [9, 10] in pure form and with chromium, iron, cobalt, nickel and cadmium as dopants. Sodium metasilicate gel of density 1.04 gem -3 was prepared and acidified with tartaric acid. The gel was allowed to set in test tubes of length 20 cm and diameter 2.5 cm. After gelation, 1 M aqueous solution of SrC12 was poured on top and allowed to diffuse into the gel. Strontium tartrate tetrahydrate crystals were found to grow in the gel. The best results were obtained for a gel density of 1.04 gcm -3, pH 4.2, 1 M tartaric acid and 1 ~ SrC12. To grow the doped crystals, an aqueous solution of the chloride of the dopant was used together with the outer reactant SrCI2. The detailed experimental procedure was reported elsewhere [11]. Doped and undoped crystals of strontium tartrate tetrahydrate of size about 8 m m × 4 mm × 2 mm (Fig. 1) were used for microhardness study. Before indentation the crystals were carefully lapped and polished to avoid surface effects which influence the hardness value strongly. Indentations were made using a Vickers pyramidal indentor for various loads from 5 to 100 g. The distance between two indentation points were more than three times the pit diagonal length, in order to avoid any mutual influence of the indentations. The diagonals of the impressions were measured using a Leitz Metallux II microscope with a calibrated ocular at magnification ×500. The measurements were made at room temperature and the indentation time was 10 s. To maintain uniformity between samples, the microhardness was measured on the dominant (1 1 0) face