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Original Articles

Size Distribution Evolution of Fine Aerosols Due to Intercoagulation with Coarse Aerosols

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Pages 358-370 | Received 04 Mar 2004, Accepted 04 Feb 2005, Published online: 23 Feb 2007

Figures & data

Figure 1 centering Various types of coagulation for bimodally distributed particles.

Figure 1 centering Various types of coagulation for bimodally distributed particles.

Table 1 Simulation conditions for studying the effects of intercoagulation on fine mode particle removal

Figure 2 Fine-mode removal time as a function of fine-mode number concentration for various coarse mode number concentrations. The solid line connects points where N f0/N c0 = 10.

Figure 2 Fine-mode removal time as a function of fine-mode number concentration for various coarse mode number concentrations. The solid line connects points where N f0/N c0 = 10.

Figure 3 centering Dimensionless removal time as a function of (a) normalized number concentration and (b) normalized mass or volume concentration.

Figure 3 centering Dimensionless removal time as a function of (a) normalized number concentration and (b) normalized mass or volume concentration.

Figure 4 centering Evolution of fine-mode (σ gf0 = 1.4) and coarse-mode (σ gc0 = 1.3) particle size distributions by intercoagulation to reach removal time (t r = 0.106 s).

Figure 4 centering Evolution of fine-mode (σ gf0 = 1.4) and coarse-mode (σ gc0 = 1.3) particle size distributions by intercoagulation to reach removal time (t r = 0.106 s).

Figure 5 Dimensionless removal time as a function of (a) fine-mode geometric standard deviation, where σ gc0 = 1.3, and (b) coarse-mode geometric standard deviation, where σ gf0 = 1.3.

Figure 5 Dimensionless removal time as a function of (a) fine-mode geometric standard deviation, where σ gc0 = 1.3, and (b) coarse-mode geometric standard deviation, where σ gf0 = 1.3.

Figure 6 (a) Dimensionless removal time and removal time as a function of d gc /d gf . (b) Dimensionless removal time as a function of fine-mode mean size.

Figure 6 (a) Dimensionless removal time and removal time as a function of d gc /d gf . (b) Dimensionless removal time as a function of fine-mode mean size.

Figure 7 (a) Removal time as a function of coarse-mode standard deviation and d gc /d gf with the same number concentration (1010/cm3) and (b) the same mass concentration (10 μ g/cm3).

Figure 7 (a) Removal time as a function of coarse-mode standard deviation and d gc /d gf with the same number concentration (1010/cm3) and (b) the same mass concentration (10 μ g/cm3).

Table 2 Size distribution parameters and removal time for CitationLinak et al. (2003)

Table 3 Operating parameters of a FGD system and particle size distribution from a power plant

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