J. Am. Ceram. Soc., 93 [2] 322–325 (2010)
DOI: 10.1111/j.1551-2916.2009.03408.x
r 2009 The American Ceramic Society
ournal
J
Synthesis and Oxidation Behavior of MgAlON Prepared from Different
Starting Materials
Guotian Ye,w Junli Shang, Dongrui Zhang, Min Liang, and Yaosheng Chen
High-Temperature Ceramic Institute, Zhengzhou University, Zhengzhou, China
The formation and oxidation of magnesium–aluminum oxynit-
ride (MgAlON) were investigated with emphasis on the effect of
impurities through using synthetic raw materials and natural
raw materials. It was observed that the formation of MgAlON
was not much influenced by the starting materials, but MgAlON
prepared from the natural starting materials exhibited acceler-
ated oxidation. The different oxidation behaviors of MgAlON
prepared from the different raw materials were discussed from
the viewpoint of impurities in the materials. The formation tem-
perature and oxidation temperature of MgAlON produced in
this work were compared with those of MgAlON prepared using
other processes.
MgAlON follows8 MgAlON1O2-MgAl2O4SS1Al2O31N2. It
was also observed13 that variation in the composition of the
MgAlON solid solution did not exert a noticeable influence on
the onset oxidation temperature and the temperature at which
a-Al2O3 began to appear.
In the above reports, monolithic MgAlON was synthesized at
temperatures between 16501 and 17001C. The earlier investiga-
tions on the oxidation behavior of MgAlON were based on
MgAlON synthesized with relatively pure starting materials,
without considering the effect of impurities. However, the use of
natural raw materials with a certain amount of impurities for the
production of synthetic raw materials for refractories is a com-
mon practice. In view of the above concern, in this work, natural
starting materials (magnesite and bauxite) with relatively higher
amounts of impurities (Fe2O3, SiO2, and TiO2) and synthetic
starting materials with relatively lower amounts of impurities
were used to prepare MgAlON, with an emphasis on the effect
of impurities. Then the synthesized MgAlON was oxidized in air
at temperatures between 11001 and 15001C to study the influ-
ence of impurities on the oxidation behavior of MgAlON.
I. Introduction
AGNESIUM–ALUMINUM OXYNITRIDE (MgAlON) possesses
M
high mechanical strength at high temperatures, high re-
sistance to slag and liquid metal,1 and good stability under room
temperature.2–4 Therefore, MgAlON can be used as high-per-
formance refractories.1,5–7 Different approaches have been used
for the synthesis of MgAlON. Dai et al.8,9 prepared MgAlON
using spark plasma sintering (SPS) at 17001C in an N2 atmo-
sphere with MgO, Al2O3, and AlN as the starting materials.
Monolithic MgAlON was produced after firing at 16501C by
carbothermal reduction and nitridation (CRN)10 of MgO,
Al2O3, and C and by a solid–gas reaction11 of Al, Al2O3, and
MgAl2O4 embedded in C and Al2O3 powders under air. Ban-
dyopadhyay et al.12 obtained monolithic MgAlON by a solid-
state reaction of MgO, AlN, and Al2O3 at 16751C in an N2
atmosphere.
II. Experimental Procedure
The samples with a higher purity (HP) were prepared with MgO,
Al2O3, and aluminum powder (Al>98 wt%, o0.074 mm) in a
molar proportion of 1.0:1.86:1.0. MgO was obtained by calci-
nation of commercial 4MgCO3 Á Mg(OH)2 Á 4H2O (ꢀ 99% pu-
rity) at 5001C and Al2O3 by calcination of commercial Al(OH)3
(ꢀ 99% purity) at 6001C. The samples with a lower purity (LP)
were composed of magnesite, bauxite, and aluminum powder in
the same MgO:Al2O3:Al molar ratio as shown above. The chem-
ical compositions of magnesite powder (o0.074 mm) and baux-
ite powder (o0.074 mm) are shown in Table I.
As mentioned above, MgAlON can be used in refractory
materials. However, MgAlON is inevitably oxidized in an oxi-
dation atmosphere at high temperatures, which would change
the phase compositions and properties of the materials contain-
ing MgAlON and consequently influence the high-temperature
performance of the material in industrial vessels. Therefore,
there has been increased interest in the oxidation behaviors of
MgAlON in recent years. It was found that oxidation of
MgAlON powder started at about 7501C,8,11 even if the oxida-
tion rate of MgAlON was very slow below 10001C.13 Although
the oxidation rate increased dramatically above 10001C from the
mass gain results of the MgAlON oxidation test, X-ray powder
diffractometry (XRD) results showed that only monolithic
MgAlON was observed at different oxidation temperatures
up to 11001C.13 Only at 12001C or above, was another phase
of a-Al2O3 detected in the oxidized product besides the cubic
spinel crystalline phase.13,14 The overall oxidation behavior of
The raw materials were meticulously weighed and mixed for
24 h in a rotary mill with zirconia balls (5 mm in diameter) using
ethanol as dispersion with a ball to powder weight ratio of 3:1.
The slurries were dried at 801C, sieved, and uniaxially pressed
under a pressure of 40 MPa to obtain cylindrical samples 20 mm
in diameter and 10 mm in height. The samples were heated with
carbon embedding to 14501 and 15501C and held for 5 h, re-
spectively, in a MoSi2 furnace under a nitrogen (99.99% purity)
atmosphere (0.02 MPa). Carbon embedding was used to keep
the oxygen partial pressure thermodynamically low enough for
the synthesis of MgAlON.14
XRD (X’Pert Pro, Philips, Eindhoven, the Netherlands) was
conducted to identify the phase compositions of the fired sam-
˚
ples using monochromatized CuKa radiation (1.54056 A). For
MgO–Al2O3 spinel, the strongest diffraction peak corresponds
to the (311) plane.15 The lattice constant of MgAlON was cal-
culated based on XRD data of the (311) plane as MgAlON has
the same cubic crystallographic structure as MgAl2O4.16 Mag-
nesium aluminate spinel (AR-78, Almatis, Ludwigshafen, Ger-
many) was used as a reference to compare with MgAlON in the
shifts of XRD peak positions. The morphology of the fired
samples was examined via scanning electronic microscopy
S. Seetharaman—contributing editor
Manuscript No. 26317. Received June 23, 2009; approved August 24, 2009.
Supported by National Natural Science Foundation of China, under Grant No.
50872125.
wAuthor to whom correspondence should be addressed. e-mail: gtye@zzu.edu.cn
322