The icosahedral quasicrystal (IQC) discovered by Shechtman et al. [1] in rapidly solidified A1-Mn alloys has a unique symmetry and striking morphology which is different from that of the crystal and is amorphous. In consequence this has stimulated considerable interest. Much work [2][3][4][5] has been concerned with identification, microstructure, composition and stability of IQC in A1-Mn alloys. Recently, some studies [6][7][8] examined the morphology of IQC formed under the different conditions, determining that the morphology of many IQC has an icosahedral symmetry, the same as the microstructures. However, a few studies centred on the formation of the unique morphology of IQC, especially on the relation between a cooling rate and morphology.We [9] ,studied the relation between the solidified morphology of IQC and the composition of the alloys, the, mean cooling rates in some A1-Mn alloys based on the published papers, and we pointed out that the morphology of IQC can be divided into three categories: equiaxial grains with a planar face, spherulites with a small protrusion and dendritic grains, which are something like that of a solidified crystal. We presented a morphological stability theory (MST) [10] which has been applied successfully in rapidly solidified (RS) crystalline alloys and can be used to predict the solidified morphology of IQC. In this paper, however, we investigated the morphology of IQC solidified at different cooling rates in an RS A1-8.2 at % manganese alloy and we analysed the formation of the unique morphology of IQC based on the stability of the solid-liquid interface and the symmetry of the microstructures. A1-8.2 at% manganese cast alloy used in this research was prepared with pure aluminium (99.99 mass %) and manganese (99.9 mass %) by melting in an argon atmosphere. Then the cast alloy was proce.ssed by melt spinning into ribbons -4 mm wide. Three different peripheral wheel speeds, v, were used to vary the ribbon thickness and ribbons B-1 to B-3, with the different cooling rates, were obtained, The values of v and thickness d of the ribbons B-1 to B-3 were summarized in Table I. The average cooling rates i# (Ks -1) of all ribbons were estimated at the 106 order of magnitude with an empirical relation between i/" and d [11]. The microstructures of each ribbon were examined with a Hitachi-450 scanning microscope (SEM) and EM-400T and an H-800 electron microscope (TEM). X-ray diffraction analysis was also made on these ribbons. Since the microstructures of a ribbon change along the cross-section, because of variation inthe cooling rate, the ribbons (before being studied in TEM) were worn off a little bit from the wheel side or the free surface of the wheel side and the free surface, respectively, so that the zone near the free surface or the zone near the wheel side or the middle zone of a ribbon could be analysed.The results of X-ray diffraction indicate that all ribbons consist of ol-A1 and IQC besides few A16 Mn in B-3 although the relative contents of IQC are different in each rib...