9
32
K. S. Rejitha, S. Mathew
Instrumentation
alternative to study the solid state reactions. Now a days
model-free isoconversional methods have gained much
attention as a useful approach to investigate the kinetics of
the solid state reactions as these methods possess several
advantages over conventional approaches [12–15]. These
methods are based on the principle that the reaction rate at
a constant extent of conversion (a) is only a function of the
temperature (T). For a single step reaction, the activation
energy (E) is constant over the whole conversion function.
For multi step kinetics, the activation energy (E) vary with
the extent of conversion and this reflects the variation in
relative contributions of single steps to the overall reaction
rate. Friedman, FWO and KAS are isoconversional
methods and are frequently employed to study the
kinetics. These methods yield effective activation energy
(E) as a function of extent of conversion (a) [16].
Thermogravimetric analyses in air were carried out using
Shimadzu DTG-60 instrument connected to a TA-60 online
analyser. The heating rates employed were 5, 10, 15 and
-
1
2
0 °C min . TG–MS studies were carried out using a
Rigaku, TG-8120 thermogravimetric apparatus combined
with mass spectroscopy (Anelva, M-QA200TS) at a heating
-
1
rate of 10 °C min
under high-purity He gas flow
(
99.9999%). For the thermogravimetric analyses, the sam-
ple mass used were 10 ± 0.2 mg for all the experiments.
The elemental analyses were carried out using Vario
Elemental III instrument. X-ray powder patterns were
recorded on a Bruker D8 Advance diffractometer using Cu
˚
Ka radiation, k = 1.542 A attached with a programmable
temperature device from Anton Paar, (TTK 450). The
measurements were performed by placing the sample on a
flat sample holder, while the samples were heated by the
programmable temperature controller. A series of diffrac-
tion patterns were recorded at every 20 °C rise of tempera-
ture. Crystallite size was calculated using Scherrer equation
In order to study the kinetics using the model-free
methods, several TG measurements were carried out at
different heating rates. Friedman, Flynn–Wall–Ozawa
(FWO) as well as KAS methods are based on multiple
heating rate experiments.
Flynn–Wall–Ozawa equation is as follows [4, 5]:
t ¼ 0:9k=bcos h;
where t is the thickness of the particle, k is the wave length,
b is full width at half maximum (FWHM) intensity
AE
E
ln / ¼ ln R ꢁ ln gðaÞ ꢁ 5:3305 ꢁ 1:052
;
ð3Þ
RT
where / is the heating rate, a is the degree of conversion, g
a) is the mechanism function, E is the activation energy, A
is the pre-exponential factor and R is the gas constant.
(
in radians) and cos h is the corresponding angle. Mor-
(
phology of the complexes, intermediates formed at differ-
ent temperatures and the residues were determined using
JEOL JSM-6390 scanning electron microscope. For SEM
analyses, the samples were spread on a carbon tape and
made uniform by blowing air.
Friedman equation is [6]:
da
E
ln ¼ ln½Af ðaÞꢂ ꢁ
;
ð4Þ
dt
RT
where dd at is the rate of conversion and f (a) is the mecha-
nism function.
Kinetic studies
Kissinger–Akahira–Sunose (KAS) equation is [7, 8]:
ꢁ
Isoconversional methods
ꢀ
/
T2
AR
E
ln
¼ ln
ꢁ
:
ð5Þ
Solid state reaction often follows the basic kinetic
equation:
EgðaÞ RT
From the above equations (3–5), plots of ln / versus 1/T,
da
dt
/
2
dðaÞ
dt
ꢁE
ln
versus 1/T, ln T
versus 1/T give straight lines with
¼
A exp
f ðaÞ;
ð1Þ
RT
slopes -1.052E/R, -E/R and -E/R, respectively, for the
FWO, Friedman and KAS equations. The slope of the
straight line is directly proportional to the activation energy.
where A is the pre-exponential factor, E is the activation
energy, R is the gas constant, T is the temperature and f (a)
is the kinetic model function. For a nonisothermal reaction,
Eq. 1 can be written as:
Results and discussion
dðaÞ
fðaÞ
A
ꢁE
dT
¼
exp
dT; where the heating rate / ¼ dt
:
ð2Þ
/
RT
Thermal decomposition studies
The above equation pertains to a single step reaction
kinetics, but quite often the solid state reactions contain
complex reaction steps and a single rate equation is unable
to explain the complexities of solid state reactions. In this
context, isoconversional methods could be used as an
Tris(ethylenediamine)nickel(II) oxalate dihydrate
The details of the elemental analyses are given in Table 1,
which are in agreement with the formulae of the
1
23