(655e) Combustion Regimes for Spark Ignited Nanocomposite Thermites
AIChE Annual Meeting
2015
2015 AIChE Annual Meeting Proceedings
Particle Technology Forum
Nano-Energetic Materials II
Thursday, November 12, 2015 - 9:54am to 10:15am
Combustion Regimes for Spark Ignited Nanocomposite Thermites
Ian Monk and Edward L. Dreizin
New Jersey Institute of Technology, Newark NJ 07102
Abstract
Four nanocomposite thermite powders prepared by arrested reactive milling, 2Al-3CuO, 2.35Al-Bi2O3,
2Al-Fe2O3, and 2Al-MoO3, were ignited by Electro Static Discharge (ESD). The powder was placed in
monolayers and in layers of 0.5 mm thickness and the effect of the layer thickness on its ignition and
combustion was studied. Using a 32-channel photomultiplier tube (PMT) coupled with a spectrometer
operating in the visible light wavelength range as well as a single PMT filtered at 568 nm, time-
dependent emission traces were recorded for the ignited materials in the wavelength range of 374.1 -
641.0 nm. Ignition delays, temporal positions of peak emission, emission peak widths, were obtained
directly from the recorded traces. The peak durations were interpreted to represent the particle burn
times. Time dependent temperatures were calculated using the recorded 32-point spectra. The
spectra were curve-fitted using Planck’s black body emission equation, considering temperature as an
adjustable parameter. The Planck’s fits were typically good for the decaying portions of the recorded
emission traces, while substantial discrepancies between the recorded spectra and the anticipated gray
body emission pattern were detected prior to the emission peak. Despite these discrepancies, the
temperatures inferred from both parts of the recorded emission traces, before and after the emission
peaks, matched with each other well. Ignited particles were captured and examined using scanning
electron microscopy (SEM).
Previously, it was reported that nanocomposite thermite powders placed in monolayers ignite and burn
as individual particles, essentially without any delay following ESD. The powders placed in 0.5-mm thick
layers were observed to ignite in two distinct regimes. In one regime, observed for 2.35Al-Bi2O3 and 2Al-
Fe2O3 powders, ignition resulted in combustion of individual particles occurring without a delay, similarly
to what observed for monolayers. For 2Al-3CuO and 2Al-MoO3, ignition occurred with delays and
resulted in a much longer and brighter cloud combustion event. Cloud combustion was occasionally
observed for 2.35Al-Bi2O3 when higher spark energies were used, but was never achieved in this work for
2Al-Fe2O3. Specific temporal characteristics of the emission pulses generated by cloud combustion were
analyzed and compared for different powders. Effect of inert gas (N2, Ar, He) on the cloud combustion
dynamics was studied for different materials. Interaction between ignited particles was found to play an
important role in the observed cloud combustion events.
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