G. Singh et al. / Thermochimica Acta 437 (2005) 21–25
25
of metal oxides (19%). Thus, the mechanism of thermolysis
may be proposed as:
Explosives, Ministry of commerce and Industry, Govt. of
India for providing lab facility at Departmental Testing Sta-
tion Gondkhairy, Nagpur for the studies on TG, DTA and
DSC.
[M(dab)2](ClO4)2xH2O → [M(dab)2](ClO4)2 + xH2O
[M(dab)2](ClO4)2 → [M(dab)](ClO4)2 + dab
[M(dab)](ClO4)2 → MO + gaseous products
The formation of monoligand intermediates has been seen
copper chloride/bromide monohydrates [31], bis(ethylene-
diamine)metal nitrate [8,11] complexes.
Comparison of the DTA and DSC exothermic peak tem-
peratures (Table 2) shows the decreasing trend as [Zn(dab)2]
(ClO4)2 ꢀ [Cu(dab)2](ClO4)2·2H2O ≈[Ni(dab)2](ClO4)2
for early thermolysis (α = 0.33).
Analysis of kinetics from isothermal TG data using model
fitting method, values of E obtained from different models for
particular sample are nearly equal irrespective of the equa-
tions used. It is difficult to assign a single value of E to a
particular process taking place in such a complex solid state
decomposition. Model-free isoconversional method shows
that the thermolysis of these complexes is not as simple as
indicated by model fitting method. As can be seen from Fig. 5,
the value of E changes with α but in all the α range, E for Zn
complex is higher than Cu and Ni which indicates the stabil-
ity of Zn complex is higher than Cu and Ni. Except in lower
α range, E for Ni is greater than Cu indicating the greater
stability of Ni over Cu complex.
To examine the effect of rapid heating on the complexes,
ignition delay was measured. A perusal of Table 2 reveals
that, at a particular temperature, τ for Cu and Ni complex are
nearly the same. This shows their similar thermal stability.
Thus, the thermal stability order is same as indicated earlier.
This thermal stability order can be directly correlated with the
cation size. Comparison of τ data for 20 and 7 mg of sample
for all three complexes indicates that it is lower for 7 mg. This
emphasizes that the self-propagative heating effect of sample
particles are less than the contact heating to the ignition tube
wall. Although the τ are different for different sample masses,
activation energies for ignition (E*) are almost the same.
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Acknowledgements
Thanks to Head, Chemistry department of DDU Gorakh-
pur University for lab facility and DRDO, ARMREB, New
Delhi for financial support. Thanks are also to Sri M.
Anbunathan, Chief Controller of Explosives, Department of
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