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Original Articles

Amplification of Light Absorption of Black Carbon by Organic Coating

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Pages 46-54 | Received 08 Apr 2009, Accepted 18 Sep 2009, Published online: 13 Jul 2010

Figures & data

TABLE 1 Measured and calculated absorption cross sections (σabs) and mass absorption cross sections (C abs) of graphite particles. The units of σabs are 10–12 m2, C abs are m2 g–1

FIG. 1 Absorption coefficient (b abs) of uncoated graphite particles with D c of 185, 234, and 281 nm. Model calculations by Mie theory are also shown.

FIG. 1 Absorption coefficient (b abs) of uncoated graphite particles with D c of 185, 234, and 281 nm. Model calculations by Mie theory are also shown.

FIG. 2 Size distribution of graphite particles (D c = 185 nm) coated by oleic acid measured with the laser of the photo-acoustic absorption spectrometer (PASS) on or off.

FIG. 2 Size distribution of graphite particles (D c = 185 nm) coated by oleic acid measured with the laser of the photo-acoustic absorption spectrometer (PASS) on or off.

TABLE 2 Terminology of effective diameters used in this study

FIG. 3 Schematic of the laboratory experiment for measuring absorption of organics-coated graphite particles. The system uses differential mobility analyzers (DMA1 and DMA2), a single particle soot photometer (SP2), and a photo-acoustic absorption spectrometer (PASS).

FIG. 3 Schematic of the laboratory experiment for measuring absorption of organics-coated graphite particles. The system uses differential mobility analyzers (DMA1 and DMA2), a single particle soot photometer (SP2), and a photo-acoustic absorption spectrometer (PASS).

FIG. 4 (a) Distribution of graphite mass-equivalent core diameter (D c) and (b) distribution of shell/core diameter ratio (D p/D c) of oleic acid-coated graphite particles with D c of 185 nm and the shell mobility diameters of 200, 300, 400, and 500 nm selected by DMA2.

FIG. 4 (a) Distribution of graphite mass-equivalent core diameter (D c) and (b) distribution of shell/core diameter ratio (D p/D c) of oleic acid-coated graphite particles with D c of 185 nm and the shell mobility diameters of 200, 300, 400, and 500 nm selected by DMA2.

TABLE 3 Uncertainties of calculated and observed absorption coefficient (b abs), mass absorption cross section (C abs), and absorption amplification factor (γ)

FIG. 5 Observed absorption amplification factor (γ) for organics-coated graphite particles with D c of (a) 185, (b) 234, and (c) 281 nm. The bottom axis shows the median of the shell/core diameter ratio (D p/D c) and the top axis shows the coating thickness (nm). Shell/core model calculations are also shown for m graphite and m graphite-air.

FIG. 5 Observed absorption amplification factor (γ) for organics-coated graphite particles with D c of (a) 185, (b) 234, and (c) 281 nm. The bottom axis shows the median of the shell/core diameter ratio (D p/D c) and the top axis shows the coating thickness (nm). Shell/core model calculations are also shown for m graphite and m graphite-air.

FIG. 6 Comparison of the b abs (Mm–1) calculated using Mie theory and that observed by PASS for (a) uncoated and (b) coated graphite particles. For coated graphite, b abs was calculated assuming the shell/core model and no absorption enhancement. The dotted 1:1 line is a visual guide.

FIG. 6 Comparison of the b abs (Mm–1) calculated using Mie theory and that observed by PASS for (a) uncoated and (b) coated graphite particles. For coated graphite, b abs was calculated assuming the shell/core model and no absorption enhancement. The dotted 1:1 line is a visual guide.

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