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Articles

Quantification of online removal of refractory black carbon using laser-induced incandescence in the single particle soot photometer

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Pages 679-692 | Received 25 Oct 2015, Accepted 02 Mar 2016, Published online: 05 Apr 2016

Figures & data

Figure 1. Experimental configuration.

Figure 1. Experimental configuration.

Figure 2. Mass-weighted size distributions of Aquadag before (solid black) and after (dashed) undergoing LII. Initial size distributions for DMA-selected mobility diameters of (a) 100 nm, (b) 150 nm, (c) 300 nm, (d) 350 nm, (e) 500 nm, and (f) polydisperse samples as detected by incandescence in the SP2. Plotted diameter is dm with residuals (ρeff = 1, dme = dm for spherical particles). Gaussian fits (gray [blue]) are used to determine the reported Sigma (σ) values.

Figure 2. Mass-weighted size distributions of Aquadag before (solid black) and after (dashed) undergoing LII. Initial size distributions for DMA-selected mobility diameters of (a) 100 nm, (b) 150 nm, (c) 300 nm, (d) 350 nm, (e) 500 nm, and (f) polydisperse samples as detected by incandescence in the SP2. Plotted diameter is dm with residuals (ρeff = 1, dme = dm for spherical particles). Gaussian fits (gray [blue]) are used to determine the reported Sigma (σ) values.

Table 1. Removal rates for Aquadag exposed to LII by mass concentration, number concentration, percent scattering, and absorption. Both the mobility-selected particle dm range as determined by ±2σ from the Gaussian fits to the original size distributions and the total particles measured by the SP2 are reported for the mass and number concentrations. Reported averages are from the mobility-selected samples, and uncertainties are the standard deviations.

Figure 4. (a) Mass and (b) number size distributions of the incandescent particles remaining after LII normalized by the original Aquadag mass and number concentrations, respectively.

Figure 4. (a) Mass and (b) number size distributions of the incandescent particles remaining after LII normalized by the original Aquadag mass and number concentrations, respectively.

Figure 3. Number size distributions of Aquadag before (solid black) and after (dashed) undergoing LII. Initial size distributions for DMA-selected mobility diameters of (a) 100 nm, (b) 150 nm, (c) 300 nm, (d) 350 nm, (e) 500 nm, and (f) polydisperse samples as detected by incandescence in the SP2. Plotted diameter is dm with residuals (ρ = 1, dme = dm for spherical particles). Gaussian fits (gray [blue]) are used to determine the reported Sigma (σ) values.

Figure 3. Number size distributions of Aquadag before (solid black) and after (dashed) undergoing LII. Initial size distributions for DMA-selected mobility diameters of (a) 100 nm, (b) 150 nm, (c) 300 nm, (d) 350 nm, (e) 500 nm, and (f) polydisperse samples as detected by incandescence in the SP2. Plotted diameter is dm with residuals (ρ = 1, dme = dm for spherical particles). Gaussian fits (gray [blue]) are used to determine the reported Sigma (σ) values.

Figure 5. (a) Mass weighted mean dme and (b) individual particle mass remaining after LII versus the original Aquadag mean dm selected with the DMA, and (c) mass mean dme after LII versus the total mass concentration of the original sample.

Figure 5. (a) Mass weighted mean dme and (b) individual particle mass remaining after LII versus the original Aquadag mean dm selected with the DMA, and (c) mass mean dme after LII versus the total mass concentration of the original sample.
Supplemental material

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