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. 2013 Dec;160(12):2996-3003.
doi: 10.1016/j.combustflame.2013.06.025.

Paramagnetic centers in particulate formed from the oxidative pyrolysis of 1-methylnaphthalene in the presence of Fe(III)2O3 nanoparticles

Affiliations

Paramagnetic centers in particulate formed from the oxidative pyrolysis of 1-methylnaphthalene in the presence of Fe(III)2O3 nanoparticles

Paul Herring et al. Combust Flame. 2013 Dec.

Abstract

The identity of radical species associated with particulate formed from the oxidative pyrolysis of 1-methylnaphthalene (1-MN) was investigated using low temperature matrix isolation electron paramagnetic resonance spectroscopy (LTMI-EPR), a specialized technique that provided a method of sampling and analysis of the gas-phase paramagnetic components. A superimposed EPR signal was identified to be a mixture of organic radicals (carbon and oxygen-centered) and soot. The carbon-centered radicals were identified as a mixture of the resonance-stabilized indenyl, cyclopentadienyl, and naphthalene 1-methylene radicals through the theoretical simulation of the radical's hyperfine structure. Formation of these radical species was promoted by the addition of Fe(III)2O3 nanoparticles. Enhanced formation of resonance stabilized radicals from the addition of Fe(III)2O3 nanoparticles can account for the observed increased sooting tendency associated with Fe(III)2O3 nanoparticle addition.

Keywords: Annealing studies; Cryogenic trapping; EPR; Environmentally Persistent Free Radicals (EPFRs); Nanoparticles; Particulate.

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Figures

Fig. 1
Fig. 1
Dual-zone reactor capable of generating metal oxide nanoparticles (Zone 1) in the presence of a high sooting 1-MN fuel (Zone 2) coupled with a cold finger for condensation of paramagnetic species. Soot was collected through a moveable probe stationed at sampling ports denoted I–IV in the isothermal region as well as sampling points A (700 °C) and B (475 °C) in the quenching zone of reactor, and sampling point C (80 °C) in the exhaust stream.
Fig. 2
Fig. 2
(A) EPR spectra of particulate accumulated at sampling port C using the cryogenic method. (B) Spectrum A on expanded scale to show detail. (C) EPR spectra of particulate collected on a cellulose-ester filter at the same sampling position.
Fig. 3
Fig. 3
(A) EPR spectra of particulate collected on Dewar cold finger. (B) EPR spectra after gradual annealing of the matrix. (C) EPR spectra after further annealing. (D) The subtraction spectrum, A and B, provides a residue spectrum of the mixture of annihilated organic radicals.
Fig. 4
Fig. 4
Power dependence of spectra of particulate collected on Dewar cold finger. At low microwave power (0.1 mW), the organic radical is resolved.
Fig. 5
Fig. 5
Normalized EPR spectra of soot particles detected in Zone 2, in the quenching zone of the reactor (ports A and B) and in the exhaust stream, port C.
Fig. 6
Fig. 6
Optimized geometries of radicals mentioned in the text; C atoms are gray, H atoms are red. On the right side; simulated spectra of radicals formed from the oxidative pyrolysis of 1-MN. The Win-EPR Simfonia simulation software was used with parameters: ΔHp–p for each individual line − 2.5 G, Lorenzian lineshape, g = 2.0030. The hyperfine splitting constants for cyclopentadienyl radical (with five equivalent protons) was 6.2 G [36]. (For interpretation of the references to color in this figure legend, the reader is referred to the web version of this article.)
Fig. 7
Fig. 7
Comparison of experimental EPR spectra with simulated spectrum composed of indeyl, cyclopentadienyl, and naphthalene 1-methylene radical. The Win-EPR Simfonia simulation software was used with parameters: ΔHp–p for each individual line − 2.5 G, Lorenzian lineshape, g = 2.0030.
Fig. 8
Fig. 8
Observed enhancement in radical formation as a result of Fe(III)2O3 nanoparticle introduction prior to soot inception.
Fig. 9
Fig. 9
Accumulated Fe(II)2O3 nanoparticles on the Dewar cold-finger exhibited the same spectral features as a ng quantity of an Fe(II)2O3 standard.

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