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Original Articles

Bipolar Diffusion Charging of Soot Aggregates

Pages 247-254 | Received 09 Dec 2007, Accepted 01 Feb 2008, Published online: 28 Apr 2008

Figures & data

FIG. 1 Schematic diagram of experimental apparatus.

FIG. 1 Schematic diagram of experimental apparatus.

FIG. 2 Typical soot size distributions used in this work: premixed ethylene flame at Φ = 2.1, sampled at 20 mm above the burner and allowed to coagulate for 1 and 20 s. Arrows illustrate the preferred relationship between size distribution and selected size for the examples of ∼ 70 nm and ∼ 250 nm particles.

FIG. 2 Typical soot size distributions used in this work: premixed ethylene flame at Φ = 2.1, sampled at 20 mm above the burner and allowed to coagulate for 1 and 20 s. Arrows illustrate the preferred relationship between size distribution and selected size for the examples of ∼ 70 nm and ∼ 250 nm particles.

FIG. 3 Charging efficiency versus aerosol flow rate through 210Po neutralizer (ADI housing) for 45 nm PAO oil droplets.

FIG. 3 Charging efficiency versus aerosol flow rate through 210Po neutralizer (ADI housing) for 45 nm PAO oil droplets.

FIG. 4 Bipolar charging of PAO oil droplets. Upper panel: z = ± 1. Lower panel: z = ± 2. Solid symbols represent experimental data from this work; open symbols are data from CitationWiedensohler et al. (1986). Solid lines represent best log-log fits of the data to third order polynomials. Dashed lines depict Fuchs model predictions.

FIG. 4 Bipolar charging of PAO oil droplets. Upper panel: z = ± 1. Lower panel: z = ± 2. Solid symbols represent experimental data from this work; open symbols are data from CitationWiedensohler et al. (1986). Solid lines represent best log-log fits of the data to third order polynomials. Dashed lines depict Fuchs model predictions.

TABLE 1 Bipolar charging efficiency parameterizations: f z = 10∑limits k a z,k log (d m ) k

FIG. 5 Triply charged particles. Top panel: PAO oil droplets. Solid lines depict Fuchs model predictions. Dashed lines are polynomial best fits. Bottom panel: flame generated soot. Solid lines are from the Fuchs model. Dashed lines show predictions from the charging theory for fibrous aerosols of CitationWen et al. (1984a) using d 0 = 17 nm.

FIG. 5 Triply charged particles. Top panel: PAO oil droplets. Solid lines depict Fuchs model predictions. Dashed lines are polynomial best fits. Bottom panel: flame generated soot. Solid lines are from the Fuchs model. Dashed lines show predictions from the charging theory for fibrous aerosols of CitationWen et al. (1984a) using d 0 = 17 nm.

FIG. 6 Bipolar charging of flame generated soot aggregates. Upper panel: z = ± 1. Lower panel: z = ± 2. Symbols represent experimental data. Solid lines depict the best fits to the spherical particle data from . Dashed lines show predictions from the charging theory for fibrous aerosols of CitationWen et al. (1984a) using d 0 = 17 nm.

FIG. 6 Bipolar charging of flame generated soot aggregates. Upper panel: z = ± 1. Lower panel: z = ± 2. Symbols represent experimental data. Solid lines depict the best fits to the spherical particle data from Figure 4. Dashed lines show predictions from the charging theory for fibrous aerosols of CitationWen et al. (1984a) using d 0 = 17 nm.

FIG. 7 TEM images of mobility size selected soot particles. (a) d m = 200 nm. (b) d m = 100 nm. (c) d m = 50 nm. (d) d m = 25 nm.

FIG. 7 TEM images of mobility size selected soot particles. (a) d m = 200 nm. (b) d m = 100 nm. (c) d m = 50 nm. (d) d m = 25 nm.

FIG. 8 Bipolar charging of diesel engine exhaust particulate matter. Upper panel: z = ± 1. Lower panel: z = ± 2. Symbols represent experimental data. Solid lines depict the best fits to the spherical particle data from . Dashed lines show predictions from the charging theory for fibrous aerosols of CitationWen et al. (1984a) using d 0 = 17 nm.

FIG. 8 Bipolar charging of diesel engine exhaust particulate matter. Upper panel: z = ± 1. Lower panel: z = ± 2. Symbols represent experimental data. Solid lines depict the best fits to the spherical particle data from Figure 4. Dashed lines show predictions from the charging theory for fibrous aerosols of CitationWen et al. (1984a) using d 0 = 17 nm.

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