First-principles interatomic potentials for transition-metal aluminides. II. Application to Al-Co and Al-Ni phase diagrams

1998 ◽  
Vol 58 (14) ◽  
pp. 8967-8979 ◽  
Author(s):  
Mike Widom ◽  
John A. Moriarty
1982 ◽  
Vol 19 ◽  
Author(s):  
A. R. Williams ◽  
C. D. Gelatt ◽  
J. W. D. Connolly ◽  
V. L. Moruzzi

ABSTRACTThe physical picture of cohesion and compound formation provided by parameter-free, self-consistent, energy-band calculations will be described. For transition-metal elements, the calculations allow us to “see” which electrons are holding the solid together and which are holding it apart. For compounds, calculated heats of formation agree well with available measurements and are in general agreement with those given by Miedema's empirical formula. (The agreement with Miedema is paradoxical, in that Miedema's conception of the formation process differs qualitatively from ours.) Preliminary, but very encouraging, results of efforts to extend the analysis to disordered materials and to the calculation of phase diagrams are described.


1996 ◽  
Vol 74 (6) ◽  
pp. 1385-1397 ◽  
Author(s):  
D. Nguyen-manh ◽  
D. G. Pettifor ◽  
G. Shao ◽  
A. P. Miodownik ◽  
A. Pasturel

Author(s):  
G.A. Botton ◽  
C.J. Humphreys

Transition metal aluminides are of great potential interest for high temperature structural applications. Although these materials exhibit good mechanical properties at high temperature, their use in industrial applications is often limited by their intrinsic room temperature brittleness. Whilst this particular yield behaviour is directly related to the defect structure, the properties of the defects (in particular the mobility of dislocations and the slip system on which these dislocations move) are ultimately determined by the electronic structure and bonding in these materials. The lack of ductility has been attributed, at least in part, to the mixed bonding character (metallic and covalent) as inferred from ab-initio calculations. In this work, we analyse energy loss spectra and discuss the features of the near edge structure in terms of the relevant electronic states in order to compare the predictions on bonding directly with spectroscopic experiments. In this process, we compare spectra of late transition metal (TM) to early TM aluminides (FeAl and TiAl) to assess whether differences in bonding can also be detected. This information is then discussed in terms of bonding changes at grain boundaries in NiAl.


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