Conclusions
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1.
The isothermal section of the Hf-Mo-C ternary system at 1400°C has been constructed.
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2.
The features distinguishing the phase equilibria at 1400°C from those in the 1700°C section are the decomposition of the binary carbide η-MoC1−x, its stabilization in the ternary system, resulting in the appearance of (γ + C) and (γ + η + C) fields, and a substantial widening of the (λ2 + β2 + 6) and (β2 + δ + α) fields, caused by the (β2 + 6) field.
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3.
The extent of the homogeneity field of the phase based on the cubic carbides (Mo, Hf)C1−x differs little, as regards both hafnium and molybdenum contents, from that at 1700°C.
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V. N. Eremenko, S. V. Shabanova, T. Ya. Velikanova, and L. A. Petrenko, “Structure of alloys and the phase equilibrium diagram of the Hf-Mo-C system (Part I),” Poroshk. Metall., No. 7, 49–56 (1975).
V. N. Eremenko, S. V. Shabanova, T. Ya. Velikanova, and L. A. Petrenko, “Structure of alloys and the phase equilibrium diagram of the Hf-Mo-C system (Part II),” Poroshk. Metall., No. 8, 45–52 (1975).
V. N. Eremenko, S. V. Shabanova, T. Ya. Velikanova, et al., “Structure of alloys and the phase equilibrium diagram of the Hf-Mo-C system (Part III),” Poroshk. Metall., No. 9, 52–57 (1975).
V. N. Eremenko, S. V. Shabanova, T. Ya. Velikanova, et al., “Structure of alloys and the phase equilibrium diagram of the Hf-Mo-C system (Part IV),” Poroshk. Metall., No. 10, 44–50 (1975).
V. N. Eremenko, S. V. Shabanova, and T. Ya. Velikanova, “Structure of alloys and the phase equilibrium diagram of the Hf-Mo-C system (Part V),” Poroshk. Metall., No. 9, 73–80 (1977).
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Translated from Poroshkgvaya Metallurgiya, No. 10(178), pp. 40–46, October, 1977.
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Eremenko, V.N., Shabanova, S.V. & Velikanova, T.Y. Structure of alloys and the phase equilibrium diagram of the Hf-Mo-C system VI. Isothermal section of the Hf-Mo-C system at 1400°C. Powder Metall Met Ceram 16, 772–777 (1977). https://doi.org/10.1007/BF00793585
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DOI: https://doi.org/10.1007/BF00793585