“…These onionlike structures are made from parallel graphene sheets arranged with their basal planes perpendicular to the radii of the structures. Ishiguro et al [11] have observed similar structures in diesel soot and di Stasio [12] makes similar observations on soot from a Bunsen burner fed by ethylene.…”
Section: Resultsmentioning
confidence: 57%
“…With the same technique, di Stasio [12] reports evidence of three different size scales in soot obtained from an ethylene flame. The early stage of soot inception has been studied recently in flamma using small-angle Xray scattering (SAXS) [13].…”
“…These onionlike structures are made from parallel graphene sheets arranged with their basal planes perpendicular to the radii of the structures. Ishiguro et al [11] have observed similar structures in diesel soot and di Stasio [12] makes similar observations on soot from a Bunsen burner fed by ethylene.…”
Section: Resultsmentioning
confidence: 57%
“…With the same technique, di Stasio [12] reports evidence of three different size scales in soot obtained from an ethylene flame. The early stage of soot inception has been studied recently in flamma using small-angle Xray scattering (SAXS) [13].…”
“…We have tested our apparatus by performing SAXS on C 60 , which has a radius of gyration of 0.363 nm, and our results agree with neutron scattering measurements. [27] We can identify three different sources for scattering at q > 1 nm -1 : the soot nuclei observed by di Stasio [15], a polycyclic hydrocarbon such as naphthalene [16], or disordered carbon with graphitic basal planes [17]. …”
Section: Resultsmentioning
confidence: 99%
“…The larger particles of this distribution correspond to polydispersed primary particles, with properties that depend upon both the radial and axial position within the flame, and that ultimately lead to a distribution with a mean radius of gyration, <R g >, of 21 nm and a polydispersity, σ S /<R g >, of 0.2, where σ S is the width of the Schultz distribution [14]. The smaller particles, which require additional experiments before they can be identified, may be the soot nuclei observed by di Stasio [15], a polycyclic aromatic hydrocarbon such as naphthalene, which we have observed [16], and/or disordered carbons with graphitic basal planes observed by Chen and Dobbins [17]. the Porod region, the scattering intensity scales as 1/q 4 and, if the system is not too polydispersed, interference fringes may be observed that will directly provide <R g > and the polydispersity, σ/<R g >, where σ is the width of the distribution.…”
“…(40) According to di Stasio, (41) carbon nanoparticles can be separated into three classes. The first is recognized as a class of primary particles (20-50 nm) that are usually reported to be subunits that make up chainlike and fractal soot aggregates.…”
This report describes an optical sensing system for fine particle detection using a combination of two techniques: laser-induced breakdown spectroscopy (LIBS) and laserinduced incandescence (LII). We have improved laser measurement systems applied for small-particle analysis. We have determined elemental composition and density of particles using LIBS and have been able to measure particle size using LII. Controlling the power density of the light source of the present system allowed switching from LIBS to LII. LII temporal analysis was conducted using a streak camera, which was also used for LIBS analysis. The LII technique allows in situ measurement of the average primary particle size of nanoscale soot particles.
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