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1 oke, forest fires, coal, gasoline and diesel soot).
2 pproximately 5% (lacey soot) to 14% (compact soot).
3 ass burning (charcoal, carbon spherules, and soot).
4 Of those, 3364 particles are soot.
5 strial, purified, pristine, and oxidized) or soot.
6 sed for LII of light-absorbing kerosene lamp soot.
7 prene to the atmospheric aging of combustion soot.
8 um absorption enhancement of 1.6x over fresh soot.
9 amorphous carbon present in arc-derived SWNT soot.
10 Printex XE2-B in relation to diesel and HVO soot.
11 ith diverse functional groups to NIST diesel soot.
12 f oxygenates that incorporate into incipient soot.
13 posed to mixtures of malathion and fullerene soot.
14 clic aromatic hydrocarbons (PAHs) content of soot.
15 s on the concentration of PAHs desorbed from soot.
16 -MS to the concentration of PAHs adsorbed on soot.
17 , C80-C2v(5), and C82-C2(5) in arc-discharge soots.
18 of the instrument (LOD(NO(2)) = 0.3 ppm, LOD(soot) = 0.54 mug m(-3), limit of detection/quantificatio
19 and the Hamaker constant was derived for the soot (1.4 x 10(-20) J) using the colloidal chemistry app
20 dioxin-like toxins from hospital incinerator soot, a common PCB oil standard and pure 2,3,7,8-tetrach
21 s measured using a three-wavelength particle soot absorption photometer (PSAP) and BC particle number
22 355 nm that correlated well with a particle-soot absorption photometer (PSAP) measuring visible ligh
23 h structural and chemical characteristics of soot account for the variability in ice nucleation effic
26 tude were measured using nanoscale spherical soot aerosol composed of aggregates with approximately 1
29 n a fluoropolymer chamber on size-classified soot aerosols in the presence of isoprene, photolyticall
32 pic growth enhance the optical properties of soot aerosols, increasing scattering by approximately 10
34 The DPF probably promotes breakout of large soot agglomerates (mostly ash-bearing) by favoring sinte
37 ntermediate (flaming) phase was dominated by soot agglomerates with AAE 1.0-1.2 and 85-100% of absorp
44 ions, both the size of primary particles and soot aggregates are found to decrease with increasing in
49 pheric aggregates are more polydisperse than soot aggregates generated from a single laboratory sourc
52 latively stable over time, especially of the soot aggregates, which had effective densities similar t
55 tioned organic phases, respectively, whereas soot, ammonium sulfate, and ammonium chloride simulated
60 al and optical signatures of the in-cylinder soot and associated low volatility organics change drama
61 tion of single-walled carbon nanotube (SWNT) soot and enrichment in high aspect ratio nanotubes are e
63 enriched in BC from historical emissions of soot and have high TOC concentrations, but the contribut
64 Kratschmer/Huffmann arc evaporated graphite soot and in the carbon material in the meteorite and imp
69 tive information on the formation process of soot and on the impact of exhausts on the environment.
70 cts of binary mixtures composed of fullerene soot and organic co-contaminants as malathion, glyphosat
74 cies may also increase the hygroscopicity of soot and strongly influence the effects of soot on regio
75 es from as-produced (AP-grade) arc discharge soot and the simultaneous enrichment in unbundled, undam
77 ise to distinguish between incidental (e.g., soot) and engineered (e.g., SWCNTs) nanoparticles, which
79 fference (due largely to solar absorption by soot) and the large magnitude of the observed surface fo
80 viously known co-occurrence of nanodiamonds, soot, and extinction is the Cretaceous-Tertiary (K/T) im
81 ng PAHs from three source materials-solvent, soot, and fuel oil-to which (3)H-benzo(a)pyrene ((3)H-Ba
82 nal and global atmospheric dispersion of the soot, and the resulting physical, environmental, and cli
84 maximally by <78% (industrial CNT) and <34% (soot) at 10.0 mg CNT/L, 5.0 mg soot/L, and diuron concen
86 udes environmental black carbon (fossil fuel soot, biomass char), engineered carbons (biochar, activa
87 mportant to link health and climate-relevant soot (black carbon) emission characteristics to specific
88 to our estimations, atmospheric emissions of soot/black C might be a smaller fraction of total PyC (<
89 bonaceous particles were generated during a "sooting burn" experiment to explore how heterogeneity in
90 extracts are easily available from fullerene soot, but finding an efficient strategy to obtain them i
91 quantifying the production and injection of soot by large-scale fires, the regional and global atmos
95 nstructed with common PAH sources (fuel oil, soot, coal tar based skeet particles) and direct spike w
96 lative humidity (RH); however, lab-generated soot coated with ammonium nitrate and held at 85% RH exh
98 .C., m(2)/g) with 1 min time resolution when soot concentrations were in the low microgram per cubic
101 With the development of organic coating, the soot core is changed from a highly fractal to compact fo
102 umber fraction of the two groups were found: soot correlated with intense traffic in a diel pattern a
104 rbon is widespread in soil due to wildfires, soot deposition, and intentional amendment of pyrolyzed
107 hydroxyl group in COME also reduced further soot emissions and decreased soot activation energy.
108 it in terms of the trade-off between NOX and soot emissions with respect to ULSD and biodiesel-diesel
109 rence with the climate system, then reducing soot emissions, thus restoring snow albedos to pristine
110 Wildfires contribute significantly to global soot emissions, yet their aerosol formation mechanisms a
115 (96% Sc3N@C80, 12 mg) have been obtained in soot extracts without a significant penalty in milligram
118 ervations help explain the larger values for soot forcing measured by others and will be used to obta
119 tility organics change dramatically from the soot formation dominated phase to the soot oxidation dom
121 3)N@C(78) has been extracted from the carbon soot formed in the electric-arc generation of fullerenes
126 nanoparticles was obtained starting with the soot generated during combustion of inexpensive paraffin
127 ack 4, and special black 6), spark discharge soot (GfG), and graphite powder was measured by a van de
128 carbon sequestration potential comparable to soot/graphite and uncharred plant biomass, respectively,
130 ations and mass accumulation rates (MARs) of soot have mainly occurred since ~1950, the establishment
132 nd black carbon (BC, in the form of char and soot), have long been recognized in modern wildfire obse
133 590) and a hydrotreated vegetable oil (HVO) soot, have been investigated using heterogeneous chemist
135 f markers, including nanodiamonds, aciniform soot, high-temperature melt-glass, and magnetic microsph
138 ght alterations in soot nanostructure, lower soot ignition temperature, and lower activation energy.
143 ained in pure form directly from as-prepared soots in a single facile step by taking advantage of the
144 ormation and properties of diesel combustion soot, including particle size distributions, effective d
145 The mass absorption cross-section of diesel soot increases with combustion temperature, being the hi
146 s new environmental problems associated with soot injection have been identified, including disruptio
148 actors for organic matter, elemental carbon (soot), inorganic species and a variety of organic compou
149 the flaming phase released large amounts of soot internally mixed with a small amount of OM, whereas
150 se dust cloud followed by fires that emitted soot into the air of New York City (NYC) well into Decem
153 dral species the complexity of the resultant soot is even greater because of the presence of multiple
155 eric circulations caused by solar heating of soot is found to stabilize the upper atmosphere against
156 Following injection into the atmosphere, the soot is heated by sunlight and lofted to great heights,
157 are highly sensitive to the manner by which soot is internally mixed with other aerosol constituents
158 t a characterization of the nanostructure of soot is needed to predict its ice nucleation efficiency.
159 om partially charred biomass and charcoal to soot) is a widely acknowledged C sink, with the latest e
161 NT) and <34% (soot) at 10.0 mg CNT/L, 5.0 mg soot/L, and diuron concentrations in the range 0.73-2990
162 The recent discovery of an apparently global soot layer at the Cretaceous/Tertiary boundary indicates
163 ere against overturning, thus increasing the soot lifetime, and to accelerate interhemispheric transp
172 bined measurements of optical properties and soot mass concentration allowed determination of mass ab
173 ybrid instrument for simultaneously tracking soot mass concentration and aerosol optical properties i
175 Particulate matter (PM) mass, number, and soot mass emissions showed strong reductions with increa
176 pproximately 2% of the starting raw nanotube soot material, significantly higher than previous method
181 se PAHs and n-alkanes, slight alterations in soot nanostructure, lower soot ignition temperature, and
182 OC) in particles, show slight alterations in soot nanostructure, reduce soot ignition temperature and
183 ining fullerenic (high tortuosity or curved) soot nanostructures arising from decreased combustion te
184 (bovine serum albumin and methylcellulose), soot, natural coastal sediments, and SWCNT-amended sedim
185 pending upon local aqueous chemistry, single soot NPs could remain stable against self-aggregation in
186 examined the aggregation behavior for diesel soot NPs under aqueous condition in an effort to elucida
188 (6)-C(82), has been isolated from the carbon soot obtained by electric arc generation of fullerenes u
189 c2C2@Cs(hept)-C88, was isolated from the raw soot obtained by electric arc vaporization of graphite r
190 The uptake coefficient for naphthalene on soot of (1.11 +/- 0.06) x 10(-5) at 293 K was determined
194 FBCs-doped fuels are effective in promoting soot oxidation and reducing the DPM mass emissions, but
198 mbination of a fast gas-sampling valve and a soot particle aerosol mass spectrometer (SP-AMS) enabled
200 uces the highest amount of soot, the highest soot particle volume, and the largest and most crystalli
201 cidate the fundamental processes that govern soot particle-particle interactions in wet environments
204 We present experimental studies to show that soot particles acquire a large mass fraction of sulfuric
206 on in flaming phase released some Cl-rich-OM/soot particles and cardboard combustion released OM and
208 ants alter the composition and properties of soot particles and lead to increased particle density, h
211 s, microscale pharmaceuticals, and nanoscale soot particles are made from rigid, aggregated subunits
212 soot produced during taxiing, where primary soot particles are smallest and most reactive and the so
215 (<5 nm), nonabsorbing coatings on nanoscale soot particles demonstrate the sensitivity of this instr
218 The morphology and internal structure of soot particles emitted from a CFM 56-7B26/3 turbofan eng
220 tic precipitator has been applied to deposit soot particles from the exhaust stream between interdigi
221 roscope imaging were applied to the in-flame soot particles inside the cylinder of a working diesel e
223 Knowledge of the morphology and mixing of soot particles is fundamental to understand their potent
224 over 90% reduction of the projection area of soot particles on the TEM image and the size of soot agg
225 The results show that the number count of soot particles per image decreases by more than 80% when
226 iled analysis shows that the number count of soot particles per image increases with increasing injec
227 ork, in particular the small size of primary soot particles present in the exhaust (modes of 24, 20,
229 ation of the mixing state of freshly emitted soot particles shows that most of them are bare (or thin
231 of internal dilation symmetry of individual soot particles subject to non-equilibrium aggregation, a
232 lts for the uptake of naphthalene (C10H8) by soot particles typical of those found in the exhaust of
233 n when polydisperse, laboratory-generated ns-soot particles were embedded within or coated with ammon
234 erated inside the engine or depict incipient soot particles which are partially carbonized in the exh
236 and the largest and most crystalline primary soot particles with the lowest oxidative reactivity.
238 M emissions that are associated with emitted soot particles, unlike the purely oil droplets observed
247 ce (HS-LII) instrument and a single particle soot photometer (SP2) were conducted upwind, downwind, a
254 ts of secondary organic aerosol formation on soot properties from OH-initiated oxidation of toluene.
256 g that even in the remote marine troposphere soot provided nuclei for heterogeneous sulfate formation
257 ences from atmospheric heating measurements, soot radiative forcing estimates currently differ by a f
259 ered EGR (FEGR) resulted in a 50% engine-out soot reduction, thus showing the possibility of extendin
260 ith a diameter smaller than 2.5 mum (PM2.5), soot (reflectance of PM2.5), nitrogen oxides (NOx), and
261 However, the late cycle soot oxidation rate (soot removal) was reduced even more, and the net effect
262 scopic characteristics of cruising condition soot resemble the ones of the approximately 100% thrust
263 final degree and coating mass dependence of soot restructuring were found to be the same for SOA coa
265 of 6, ranging between 0.2-1.2 W/m(2), making soot second only to CO(2) in terms of global warming pot
267 test vehicle was equipped with the AVL Micro Soot Sensor (photoacoustic soot sensor) to prove the con
268 ith the AVL Micro Soot Sensor (photoacoustic soot sensor) to prove the conductometric sensor principl
269 an important role in aging of anthropogenic soot, shortening its atmospheric lifetime and considerab
271 efficient measurements from a Photo Acoustic Soot Spectrometer were used to estimate aerosol optical
273 Here we report the ubiquitous presence of soot superaggregates (SAs) in the outflow from a major w
274 gest oxidization of SO2 may have occurred on soot surfaces, implying that even in the remote marine t
275 orcing from aerosols is due to black carbon--soot--that is released from the burning of fossil fuel a
276 njection into the atmosphere of 15,000 Tg of soot, the amount estimated to be present at the Cretaceo
277 and NOx models were correlated with personal soot, the component least affected by indoor sources.
278 y 100% thrust produces the highest amount of soot, the highest soot particle volume, and the largest
279 compared to the results from diesel and HVO soot, the latter being the one with the largest abundanc
281 groscopicity, and further exposure of coated soot to elevated relative humidity results in a more sph
285 agnetic microspherules, (iii) charcoal, (iv) soot, (v) carbon spherules, (vi) glass-like carbon conta
286 fference in dispersive interactions with the soot versus with the water was the dominant factor encou
288 y stems from the fact that the actual amount soot warms our atmosphere strongly depends on the manner
290 Diesel traffic-related elemental carbon (EC) soot was also associated with IHD mortality (HR = 1.03;
292 ited in Linsley Pond, Connecticut, USA while soot was more abundant during the warmer and drier early
293 a on emission factors of OC and EC (char and soot) was assessed for four cookstoves (advanced, improv
298 obtained from the analysis of flame sampled soot with standard commercial GC-MS run in parallel vali
299 ism of atmospheric aging, internal mixing of soot with sulfuric acid has profound implications on vis
300 tion in terms of EFs for OC and EC (char and soot) within the cooking cycle was also found to be sign
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