Phase Relations and Crystal Structure of 蟿6-Ti2(Ti0.16Ni0.43Al0.41)3
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Ti2(Ti0.16Ni0.43Al0.41)3 is a novel compound (labeled as 蟿6) in the Ti-rich region of the Ti鈭扤i鈭扐l system in a limited temperature range 870 < T < 980 掳C. The structure of 蟿6-Ti2(Ti,Ni,Al)3 was solved from a combined analysis of X-ray single crystal and neutron powder diffracton data (space group C2/m, a = 1.85383(7) nm, b = 0.49970(2) nm, c = 0.81511(3) nm, and 尾 = 99.597(3)掳). 蟿6-Ti2(Ti,Ni,Al)3 as a variant of the V2(Co0.57Si0.43)3-type is a combination of slabs of the MgZn2-Laves type and slabs of the Zr4Al3-type forming a tetrahedrally close-packed Frank鈭扠asper structure with pentagon鈭抰riangle main layers. Titanium atoms occupy the vanadium sites, but Ti/Ni/Al atoms randomly share the (Co/Si) sites of V2(Co0.57Si0.43)3. Although 蟿6 shows a random replacement on 6 of the 11 atom sites, it has no significant homogeneity range (1 at. %). The composition of 蟿6 changes slightly with temperature. DSC/DTA runs (1 K/min) were not sufficient to define proper reaction temperatures due to slow reaction kinetics. Therefore, phase equilibria related to 蟿6 were derived from X-ray powder diffraction in combination with EPMA on alloys, which were annealed at carefully set temperatures and quenched. 蟿6 forms from a peritectoid reaction 畏-(Ti,Al)2Ni + 蟿3 + 伪2 鈫?蟿6 at 980 掳C and decomposes in a eutectoid reaction 蟿6 鈫?畏 + 蟿4 + 伪2 at 870 掳C. Both reactions involve the 畏-(Ti,Al)2Ni phase, for which the atom distribution was derived from X-ray single crystal intensity data, revealing Ti/Al randomly sharing the 48f- and 16c-positions in space group Fdm (Ti2Ni-type, a = 1.12543(3) nm). There was no residual electron density at the octahedral centers of the crystal structure ruling out impurity stabilization. Phase equilibria involving the 蟿6 phase have been established for various temperatures (T = 865, 900, 925, 950, 975 掳C, and subsolidus). The reaction isotherms concerning the 蟿6 phase have been established and are summarized in a Schultz鈭扴cheil diagram.

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