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Original Articles

Characterization of an Automated, Water-Based Expansion Condensation Nucleus Counter for Ultrafine Particles

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Pages 1174-1183 | Received 09 Jun 2005, Accepted 24 Oct 2005, Published online: 23 Feb 2007

Figures & data

FIG. 1 Dependence of Saturation ratio after expansion with temperature before expansion according to Equations (Equation1) and (Equation2) (solid curve). Kelvin diameter versus temperature before expansion for a given saturation ratio according to Equation (Equation3) (dotted curve) for water.

FIG. 1 Dependence of Saturation ratio after expansion with temperature before expansion according to Equations (Equation1) and (Equation2) (solid curve). Kelvin diameter versus temperature before expansion for a given saturation ratio according to Equation (Equation3) (dotted curve) for water.

FIG. 2 Schematic diagram of scattered light detection with the Expansion-CNC. Particles inside an expansion chamber scatter incoming laser light. The direct light beam and the scattered light in the forward direction between 0° and 1.1° are blocked. Scattered light that hits the annular area of a lens between 1.1° and 4.4° (shaded area) is collected and focused onto a photo diode detector.

FIG. 2 Schematic diagram of scattered light detection with the Expansion-CNC. Particles inside an expansion chamber scatter incoming laser light. The direct light beam and the scattered light in the forward direction between 0° and 1.1° are blocked. Scattered light that hits the annular area of a lens between 1.1° and 4.4° (shaded area) is collected and focused onto a photo diode detector.

FIG. 3 Diagram of the Expansion-CNC. The dotted rectangle depicts the optical part of the instrument that is usually covered by a light-absorbing box.

FIG. 3 Diagram of the Expansion-CNC. The dotted rectangle depicts the optical part of the instrument that is usually covered by a light-absorbing box.

FIG. 4 Comparison of experimental (a) and theoretical (b) scattered light intensity. The vertical lines indicate the maximum and the minimum of the third step, respectively.

FIG. 4 Comparison of experimental (a) and theoretical (b) scattered light intensity. The vertical lines indicate the maximum and the minimum of the third step, respectively.

TABLE 1 Radius range at which a step can be observed and the corresponding average total and partial scattering cross section

FIG. 5 Experimental set-up for comparison of the TSI UCPC and the Expansion-CNC.

FIG. 5 Experimental set-up for comparison of the TSI UCPC and the Expansion-CNC.

FIG. 6 Comparison of measured and modeled curve for two different number concentrations. Modeled curve is calculated for monodisperse particles.

FIG. 6 Comparison of measured and modeled curve for two different number concentrations. Modeled curve is calculated for monodisperse particles.

TABLE 2 Concentration ranges that can be measured with a certain step

FIG. 7 Comparison of measured and modeled curve for an extinction experiment. Observed and modeled ripple structures are in very good agreement. For clarity the modeled curve is shifted upwards by 0.003.

FIG. 7 Comparison of measured and modeled curve for an extinction experiment. Observed and modeled ripple structures are in very good agreement. For clarity the modeled curve is shifted upwards by 0.003.

FIG. 8 Comparison of the number concentration measured by the Expansion-CNC and by the TSI UCPC for two lab-generated aerosol types.

FIG. 8 Comparison of the number concentration measured by the Expansion-CNC and by the TSI UCPC for two lab-generated aerosol types.

FIG. 9 Comparison of the number concentration measured by the Expansion-CNC and by the TSI UCPC for ambient aerosol particles.

FIG. 9 Comparison of the number concentration measured by the Expansion-CNC and by the TSI UCPC for ambient aerosol particles.

TABLE 3 Summarized characteristics of the Expansion-CNC

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