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−
1
−
E
RT
αβ
α
d
d
α
α
(2.31)
f
()
=
A
exp
,
α
T
a
where
E
ʱ
is estimated by an isoconversional method,
A
ʱ
is evaluated via the com-
pensation effect, and
T
ʱ
and (d
ʱ
/d
T
)
ʱ
are experimental values measured at the heat-
ing rate
ʲ
. Substitution of the values into Eq. 2.31 yields numerical values of
f
(
ʱ
),
which can further be matched to the theoretical
f
(
ʱ
) models (Fig. 1.4).
Figures
2.13
and
2.14
exemplify the application of the aforementioned method
in the case of thermal dehydration of nedocromil sodium trihydrate that occurs in
two well-separated steps [
64
]. For both steps, the
E
ʱ
values estimated by an isocon-
versional method do not demonstrate practically any dependence of
ʱ
(Fig.
2.13
).
The compensation effect (Eq. 2.29) has been used to estimate the
A
ʱ
values, which
were substituted in Eq. 2.30 to evaluate the reaction model,
g
(
ʱ
) in numerical form
(points in Fig.
2.14
). Comparison of the
g
(
ʱ
) values against the theoretical reaction
models suggests that the first step of dehydration follows the zero-order reaction
model,
g
(
ʱ
) =
ʱ
(R1).
However, for the second dehydration step, the
g
(
ʱ
) values fall between two dif-
fusion models D2 and D3 (Table 1.1). This is not very unusual considering the
Fig. 2.13
E
ʱ
values estimated by an isoconversional method for first (
diamonds
) and second (
tri-
angles
) steps of dehydration of nedocromil sodium trihydrate. (Reproduced from Zhu et al. [
64
]
with permission of Wiley)
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