168 Materials Science and Engineering, A 179/A 180 (1994) 168-172
A study of the glass-forming range in the ternary Ti-Ni-A1 system by
mechanical alloying
R. Nagarajan and S. Ranganathan
Centre for Advanced Study, Department of Metallurgy, Indian Institute of Science, Bangalore .560 012 (India)
Abstract
The glass-forming range (GFR) in ternary Ti-Ni-Al alloys was determined via mechanical alloying using a high energy
Spex mill. The GFR was also calculated using Miedema's model. Although the theoretical GFR is quite large, the experi-
ments showed a very limited GFR. The concentration ranges chosen were TisoNixAls0_* (x = 10, 25, 40), Ti60Ni~Al4, ,
(y = 10, 20, 30), TiToNitsA115, NizTiA1 and TiNiAI. Prolonged milling of the amorphous TisoNi25A125powders led to the
reappearance of the crystalline peaks. Calorimetric experiments showed an endothermic peak near 600 K in most of the
samples.
1. Introduction
Among non-equilibrium processing techniques,
mechanical alloying has gained popularity over rapid
solidification processing techniques in recent years
since it promises the possibility of production in bulk
amounts. Mechanical alloying is a solid state reaction
process, where a large glass-forming range is achieved
[1]. There are excellent proceedings available on the
types of metastable microstructure that can form
during mechanical alloying [2, 3].
Suryanarayana and co-workers [4, 5] have listed the
various possible metastable microstructures in titanium
base alloys achievable by rapid solidification process-
ing and mechanical alloying. Considerable work has
been reported on the mechanical alloying of Ti-Ni
[6-8] and Ti-Al [9, 10] systems. The formation of
nanocrystalline phases has been observed in these
systems [11]. However, very few reports are available
on ternary systems. Ti-Ni-Cu [8, 12-14], Ti-Cu-Pd
[15] and Ti-Ni-A1 [16] have been studied. Detailed
studies of both Ti-Ni [8, 17] and Ti-Ni-Cu [8] during
mechanical alloying and rapid solidification processing
have been carried out in our laboratory. The Ti-Ni-Cu
system has a deep eutectic which suggests a large heat
of mixing for the liquid. It showed a fairly large glass-
forming range during mechanical alloying. Other than
the binary intermetallic compounds, A16.sNiTi2. 5,
Al2NiTi, AINiTi and A1Ni2Ti are present in the
Ti-Ni-A1 system [18].
Itsukaichi et al. [16] determined the glass-forming
range in the Ti-Ni-A1 system using a conventional ball
mill. It was deduced that the composition close to
Ti6vNi33 could be easily amorphized, whereas at com-
positions close to the pure metals, the alloys give only
solid solutions. Also, an AINi type structure is reported
close to the A1Ni binary side. They reported a phase
which has an f.c.c, structure (E93) similar to that of
Ti2Ni in a vacuum hot pressed TisoNi25A125 sample.
Since the Ti-Ni, A1-Ni and Ti-A1 binary systems
have important intermetallic compounds, and since
Ti-A1 and Ti-Ni show a wide range of amorphous
phases during mechanical alloying, the Ti-Ni-AI
system is an obvious choice for study of the glass-
forming range. The model used by Murty et al. [8] was
used to obtain the glass-forming range theoretically in
the Ti-Ni-A1 system and this is compared with the
experimental results of the present work obtained
using a high energy Spex mill.
2. Experimental procedure
High purity (greater than 99.95%) titanium, nickel
and aluminium powders with particle sizes of approxi-
mately 325 mesh (less than 45 × 103 nm) were used for
our study. The powders were thoroughly mixed in a
high energy Spex mill. This is a vibratory mill in which
the vial vibrates in three mutually perpendicular direc-
tions with an amplitude of 50 mm and a frequency of
20 Hz. The speed of the mill used was 1200 rev min- ~.
Steel balls of 15 mm diameter were used and the ball to
powder ratio taken was 8:1. The kinetic energy per
ball is 0.14 J.
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