Phase Diagram Relationships in the Ternary System Ti-Ai-V

1990 ◽  
Vol 213 ◽  
Author(s):  
Mohan Paruchuri ◽  
T.B. Massalski

ABSTRACTLiquid-solid and solid state phase equilibria in the ternary system Ti-Al-V have been studied using a combination of several experimental techniques. A likely surface of primary seperation (i.e., the liquidus surface) is proposed in the form of the usual projection on the triangular base and the directions of the monovariant lines are defined. Four ternary invariant reactions have been identified in this system. Solid state equilibria have been determined at 900°C and are presented in the form of an isothermal section through the phase diagram. These are very similar to the relationships reported at 800°C by Hashimoto et al. [1].

1998 ◽  
Vol 552 ◽  
Author(s):  
B. P. Bewlay ◽  
J.-C. Zhao ◽  
M. R. Jackson ◽  
R. R. Bishop

ABSTRACTIn-situ composites based on Nb-Si alloys are potential candidates for application as structural materials in future aircraft engines. In order to achieve the balance of properties that is required, additional alloying species, such as Ti, Hf, Mo, Cr, Al, are employed. The present paper describes the effect of Hf additions on phase stability of Nb-Si alloys. Liquid-solid and solid-state phase equilibria have been investigated. The Nb-Hf-Si liquidus surface and the isothermal section at 1500°C will be described. A broad range of Nb and Hf compositions were investigated for Si concentrations up to 35.0%.


1979 ◽  
Vol 34 (4) ◽  
pp. 430-436 ◽  
Author(s):  
W. Piekarczyk ◽  
W. Weppner ◽  
A. Rabenau

A solid state galvanic cell technique has been employed to determine the phase diagram of the ternary system Y-Fe-O in the temperature range from 900 to 1250 °C. Only electrical quantities need to be measured and the samples do not have to be quenched. YFeO3 and Y3Fe5O12 exist over the entire temperature range, whereas the third ternary compound YFe2O4-x is only thermodynamically stable above 1010 ± 9 °C. Above 1078 ± 15 °C YFe2O4-x comes into equilibrium with Y2O3.With the same experimental arrangement the standard Gibbs free energies of formation ⊿G f0 of the ternary compounds YFeO3, Y3Fe5O12 and YFe2O4 have been determined to be -1366.0 + 0.2525 X T kJ/mol (1173 ≦ T [K] ≦ 1523), - 4912.2 +0.9990 X T kJ/mol (1173≦T[K] ≦ 1523) and -1615.9 + 0.3068 x T kJ/mol (1283≦T[K] ≦ 1523) as functions of the temperature, respectively


2005 ◽  
Vol 7 (6) ◽  
pp. 780-783 ◽  
Author(s):  
Henri Noël ◽  
Olivier Tougait ◽  
Robert Troc ◽  
Vasyl Zaremba

ChemInform ◽  
2015 ◽  
Vol 46 (50) ◽  
pp. no-no
Author(s):  
Bernard Marciniak ◽  
Volodymyr Pavlyuk ◽  
Ewa Rozycka-Sokolowska ◽  
Lukasz Karwowski ◽  
Zygmunt Bak

2020 ◽  
Vol 41 (3) ◽  
pp. 282-298
Author(s):  
Peter Kainzbauer ◽  
Martin C. J. Marker ◽  
Klaus W. Richter

Abstract The binary manganese–rhodium (Mn–Rh) phase diagram was reinvestigated from 5 to 90 at.% Rh with focus on determining the transition temperature between the ordered γ′-Mn3Rh and the γ-Mn phase as well as the transition temperature between of the tetragonal and cubic MnRh phase and phase boundaries, applying XRD, DTA and SEM including EDX. A reassessment of the Mn–Rh phase diagram based on obtained and literature data is given. Furthermore, the phase equilibria of the ternary bismuth–manganese–rhodium (Bi–Mn–Rh) system were experimentally investigated, focusing on the possible existence of new ferromagnetic phases. Isothermal sections at 330 °C and 600 °C were studied applying powder XRD and EDX. The corresponding phase diagram was established based on these results. No additional ferromagnetic phase was found in the ternary system.


2020 ◽  
Vol 844 ◽  
pp. 155754
Author(s):  
M. Saidi ◽  
K. Nouri ◽  
S. Walha ◽  
L. Bessais ◽  
M. Jemmali

2009 ◽  
Vol 481 (1-2) ◽  
pp. 301-304 ◽  
Author(s):  
H. Zhifeng ◽  
G. Zhengfei ◽  
C. Gang ◽  
H. Qingyan ◽  
Z. fuqiang ◽  
...  

2017 ◽  
Vol 69 ◽  
pp. 7-12
Author(s):  
L.O. Fedyna ◽  
A.O. Fedorchuk ◽  
V.M. Mykhalichko ◽  
Z.M. Shpyrka ◽  
M.F. Fedyna

ChemInform ◽  
2009 ◽  
Vol 40 (3) ◽  
Author(s):  
Y. H. Zhuang ◽  
X. Chen ◽  
J. L. Yan ◽  
C. H. Ma ◽  
K. F. Li

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