669.017.3.295N24N793N Physicochemical analysis methods have been applied to TiNi − Ni − Sc 1.13 Ni alloys at 900°C. It is shown that the phase interactions under these conditions are unaltered by comparison with those at subsolidus temperatures. The phase based on TiNi 3 , which is the most thermally and thermodynamically stable, is in equilibrium with all the other phases in the TiNi − Ni − Sc 1.13 Ni subsystem. The solubilities of the components in the phases based on Ti 50−x NiSc x , TiNi 3 , and the Laves phase are reduced at 900°C. The temperature of the polymorphic transformation in the phase based on ScNi 5 is raised by the dissolution of titanium in it to 930°C. An isothermal section is constructed of the phase diagram for the TiNi − Ni − Sc 1.13 Ni subsystem together with two polysections.Phase equilibria have been examined [1,2] in the Ni − Sc − Ti system in the TiNi − Ni − Sc 1.13 Ni region on the crystallization of alloys and at subsolidus temperatures. This paper continues the results on Ni − Sc − Ti alloys and represents the alloy structure at 900°C.Interest in alloys in the Ti − Ni system is related to their phase diagram, which has been subject to repeated transformation and refinement. To derive an optimized description of the phases in the Ti − Ni system [3], we have used data not previously available and which were not employed in discussing the results in [1, 2], from which we have considered the thermodynamic evaluation of the phase equilibria in this system and the description of the nonstoichiometry of phases based on TiNi and TiNi 3 . In accordance with [3], the phase based on TiNi 3 and considered to be a linear has a region of homogeneity on the nickel side: 5 at.% at subsolidus temperature and 2 at.% at 900°C. The other elements in the phase equilibria characterizing the Ti − Ni system behave in accordance with the model given in [4]. The solubility of nickel in TiNi at 900°C is close to 3 at.%; that of titanium in nickel is close to 11 at.%; and that of nickel in titanium is close to 10 at.%.The homogeneity regions of all the phases in the Sc − Ni system, with the exception of the Laves phase ScNi 2 , are less than 1 at.%. The homogeneity region at 900°C is in the interval 28-34 at.% Sc [5]. The binary phase based on ScNi 5 undergoes a polymorphic transformation at 880 ± 20°C [6, 7]. Its high-temperature modification has a hexagonal crystal structure of CaCu 5 type, while the structure of the low-temperature phase has not been established. The phase diagram for the Ni − Sc − Ti system can be triangulated along the section between the equiatomic phases in the binary systems Ni − Ti and Ni − Sc [1,2,8]. At 900°C, the NiTi − Sc 1.13 Ni section is quasibinary.See [1, 2, 8] on the purity of the initial components, the preparation conditions, and the methods of examining the Ni − Sc − Ti alloys. After homogenization at subsolidus temperatures [2], the Ni − Sc − Ti alloys were annealed at 900°C for 50 h in an oven filled with argon. This gave the isothermal section at 900°C for the Ni − Sc − ...