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Face-centered-cubic to hexagonal-close-packed
transformation in nanocrystalline Ni(Si) by
mechanical alloying
M.K. Datta, S.K. Pabi, and B.S. Murty
a)
Department of Metallurgical and Materials Engineering, Indian Institute of Technology,
Kharagpur-721 302, India
(Received 7 August 1999; accepted 27 March 2000)
An allotropic transition from face-centered-cubic (fcc) to hexagonal-close-packed (hcp)
Ni(Si) solid solution in Ni
95
Si
5
and Ni
90
Si
10
during nanocrystallization by mechanical
alloying is reported. The transformation was identified as a defect-induced melting
accompanied by a volume expansion of 8.6% and was observed when fcc Ni(Si)
reached a critical crystallite size of 10 nm. Calculation based on equation of state
showed that a 37% reduction in tetragonal shear modulus and a negative pressure of
about 8.7 GPa were generated at the onset of transformation.
Crystal to amorphous transformation can be induced in
a wide range of materials by various solid-state tech-
niques such as high-energy particle irradiation, ion-beam
mixing, annealing of diffusion couples, hydrogen charg-
ing, and high-energy ball milling.
1,2
Despite this variety
of techniques, there appears a common observation that
atoms are displaced from their equilibrium lattice sites,
causing lattice strain and softening of shear elastic con-
stants during the progress of amorphization.
2
According
to Lindemann’s melting criterion and the unified ap-
proach of melting and amorphization,
3
amorphization
would occur when the root-mean-square static atomic
displacement reaches a critical value identical at the
melting point of the crystal. On the other hand, Tallon
4
has pointed out that shear elastic constant falls rapidly
with an increase in crystal volume and reaches zero at a
volume equal to that of the liquid at the melting point.
The experimental results
5
have identified that amorphiza-
tion occurs when the crystal is strained to a material-
dependent critical value, and accompanies a large
decrease (∼40 to 50%) in the shear elastic constant irre-
spective of the material. The prerequisities of this phase
transformation, namely, the static atomic displacement
and shear softening, can be obtained by the presence of
static disorder in the parent crystal that can be achieved
either by accumulation of defects or by forming a super-
saturated solid solution by various solid-state techniques.
Mechanical deformation during mechanical alloying
(MA) involves the creation and annihilation of a high
density of dislocation in the material, resulting in
nanocrystalline grains of a special type of grain bound-
ary.
6
As the atomic displacement in the nanocrystalline
grain boundary is higher than the interior of the core, it is
expected that the grain boundaries have significant effect
on shear softening to induce phase transformation in the
nanocrystalline state. Therefore, it becomes possible that
the nanocrystalline grain surrounded by a disordered
layer may transform to amorphous or other crystal struc-
ture below a critical crystallite size. Experiments have
shown that nanoparticles of a number of elements such as
Nb, Mo, Co, W, Ta,
7
and less common metals such as Y,
Gd, Tb, Dy, Ho, Er, and Tm
7
have shown structures other
than their equilibrium ones. It is well known that face-
centered-cubic (fcc) Ni does not show any polymorphism
in the bulk state. However, ion irradiation studies
8,9
demonstrated that Ni can have a metastable hexagonal-
close-packed (hcp) structure. The phase transitions from
loose-packed structures to close-packed structures during
nanocrystallization can be understood by thermodynamic
consideration.
7
However, the transitions between close-
packed structures are less studied.
10
The present study
reports the formation of hexagonal phase on nanocrys-
tallization during mechanical alloying of Ni
95
Si
5
and
Ni
90
Si
10
and a possible mechanism for this phase trans-
formation is suggested.
Pure Ni and elemental blends of Ni and Si powders of
nominal composition Ni
95
Si
5
and Ni
90
Si
10
were sub-
jected to high-energy ball milling using a planetary ball
mill (Fritsch Pulverisette P-5, Fritsch GmbH, Idar-
Oberstein, Germany). The milling was carried out in
toluene at 300 rpm up to 50 h in a tungsten carbide vial
using 10-mm-diameter tungsten carbide balls with a ball-
to-powder weight ratio of 10:1. The milling was inter-
rupted at regular intervals of 5 h to analyze the milled
a)
Present address: National Research Institute for Metals, Tsukuba
305-0047, Japan.
J. Mater. Res., Vol. 15, No. 7, Jul 2000 © 2000 Materials Research Society 1429