Effect of SHS conditions on microstructure of NiTi shape memory alloy
Graphical abstract
Introduction
Approximately equimolar Ni–Ti alloy is the most widely known shape memory alloy. Shape memory effect in this alloy is connected with the transformation between austenite (high-temperature modification having B2 cubic structure) and low-temperature monoclinic martensite [1]. For the practical application of these alloys, superelasticity is very important. This phenomenon occurs when the NiTi alloy is deformed slightly above the martensite → austenite transformation temperature. Deformation induces the formation of the martensite phase, which is continuously transformed to austenite during unloading. Due to this phenomenon, this alloy behaves like enormously elastic material [1].
The transformation temperatures in NiTi alloy depend greatly on the content of nickel as well as on the amount of impurities. The impurities in NiTi alloy can be also present in the form of inclusions, such as TiN of TiC, that arise during the metallurgical processing [2], [3].
The most commonly applied techniques in industrial production of nitinol alloy are melting metallurgy processes – vacuum induction melting (VIM) [3], [4] and vacuum arc re-melting (VAR) [5]. In VIM of Ti-containing alloys, there is a serious danger of a strong contamination of the melt due to high reactivity of molten titanium. Therefore, special zirconia (ZrO2) or yttria (Y2O3) bulk or coated crucibles have to be applied [6]. However, even these materials contaminate the molten NiTi alloy partially, causing the presence of oxide inclusions. The VAR technique enables to prepare alloys with higher purity, but the problem is homogeneity. To obtain sufficiently homogenous product, the VAR process has to be repeated even more than 4 times [4], [5].
A promising alternative to these melting metallurgy production routes is powder metallurgy (PM). However, the application of conventional PM processes using NiTi alloy powders is complicated due to their poor compressibility and sinterability [4]. As the compaction methods, advanced consolidation techniques such as hot isostatic pressing or spark plasma sintering are required [4]. Alloyed powders prepared by the methods involving melting (e.g. melt atomization) can be also contaminated by the same elements as the melting metallurgy product.
A simple alternative production technology is reactive sintering. In general, reactive sintering is a densification process, where initial components in powder form are transformed to a compact product via thermally-activated chemical reactions [7]. Since the intermetallics-forming reactions are strongly exothermic, the heat evolved by the reaction sustains and propagates the reaction through the reaction mixture. Therefore the process is called SHS (Self-propagating High-temperature Synthesis) [7], [8], [9]. The route from powders to the compact usually concerns powder blending, cold pressing and sintering [7], [10]. In some processes, cold pressing and reactive sintering are replaced by reactive hot isostatic pressing [4]. The energy for the activation of chemical reactions during reactive sintering is supplied by heating in vacuum or protection-atmosphere furnace [7], [8], [9] or by electric discharge [11]. When pure metallic powders are applied and the process is carried out in vacuum or protective atmosphere to prevent oxidation, this technique enables to yield high-purity materials. In addition to high purity, controlled porosity can be also achieved, when NiTi is produced by this process [12], [13]. The porosity in SHS process was found to be formed by several phenomena: thermal migration, volume change [14] due to the crystal lattice re-ordering [14], [15], Kirkendall effect [15], gas porosity [7] or residual porosity after pressing [16]. On the contrary to the papers dealing with porous NiTi, this work aims to develop the SHS production route for low-porosity high-purity NiTi alloy.
Section snippets
Experimental
The dependence of microstructure of NiTi shape memory alloy on reactive sintering conditions was studied in this work. The chemical composition of the alloy was.
50 at.% Ni and 50 at.% Ti. Alternatively, the increase of the nickel content in the alloy to 60 at.% was also tested. Experimental material was prepared by blending of nickel powder (particle size <10 μm, > 99.8% purity, supplied by Merck), and titanium powder of various fractions in the proportions given above. Fine commercial titanium
Results and discussion
In our previous works [15], [23] it has been proved that the heating rate strongly affects the SHS process. High heating rates (over 300 °C min−1) are required to obtain NiAl or FeAl based materials, while in several systems (as TiAl–Ti5Si3 in-situ composites), heating rates achievable by common electric resistance heating (20–50 K.s−1) are sufficient. In all of the above mentioned systems, the increase of the heating rate lowers the porosity and the amount of unreacted components. However, the
Conclusions
In this paper, the effect of various SHS parameters on the microstructure, phase composition and porosity of the product was investigated. It was shown that heating rate strongly affects the structure of this alloy. The microstructure consisting of NiTi and Ti2Ni phases can be obtained in this material by rapid heating (over 300 °C min−1) only. Sufficient reactive sintering temperature to obtain NiTi phase is 900 °C. Further increase of the SHS initiation temperature to 1100 °C reduces porosity
Acknowledgement
This research was financially supported by Czech Science Foundation, project No. P108/12/G043. Přemysl Beran wants to thanks for the support from the CANAM infrastructure.
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