Figures & data
Figure 1. Transmission electron microscopy analysis of particle morphology for the hydrophobic (NM-103) and hydrophilic (NM-104) TiO2 aerosols.
![Figure 1. Transmission electron microscopy analysis of particle morphology for the hydrophobic (NM-103) and hydrophilic (NM-104) TiO2 aerosols.](/cms/asset/b5e254bc-a563-44c7-9be3-f97785c5cd3d/uast_a_1216072_f0001_b.gif)
Figure 2. Particle number size distributions of the aerosols generated using two types of nanopowder: left, hydrophobic TiO2; right, hydrophilic TiO2 (no critical orifice, RH = 0%).
![Figure 2. Particle number size distributions of the aerosols generated using two types of nanopowder: left, hydrophobic TiO2; right, hydrophilic TiO2 (no critical orifice, RH = 0%).](/cms/asset/e02e6bdc-4d6d-4ee4-b4f2-2cdb69b3813a/uast_a_1216072_f0002_b.gif)
Figure 3. Effects of a pressure drop and relative humidity on the mean particle diameter and total number concentration of hydrophobic (NM-103) and hydrophilic (NM-104) TiO2 aerosols. Total particle number concentrations are shown using relative scales, compared to the standard test conditions (0% RH and 0 kPa).
![Figure 3. Effects of a pressure drop and relative humidity on the mean particle diameter and total number concentration of hydrophobic (NM-103) and hydrophilic (NM-104) TiO2 aerosols. Total particle number concentrations are shown using relative scales, compared to the standard test conditions (0% RH and 0 kPa).](/cms/asset/b20c8c74-2a89-4a87-be4d-4254b8b4b2ba/uast_a_1216072_f0003_oc.gif)
Figure 4. Effects of pressure drops on particle number fractions in three different size ranges (<100 nm, 100–350 nm, and >350 nm) for hydrophobic (NM-103) and hydrophilic (NM-104) TiO2 aerosols.
![Figure 4. Effects of pressure drops on particle number fractions in three different size ranges (<100 nm, 100–350 nm, and >350 nm) for hydrophobic (NM-103) and hydrophilic (NM-104) TiO2 aerosols.](/cms/asset/3023b2e2-a17e-437c-ac44-ae7e96673e10/uast_a_1216072_f0004_oc.gif)
Figure 5. Changes in particle numbers (%) in individual size channels (measured by SMPS) by increasing 1% relative humidity (left) and by increasing 1 kPa pressure drop (right). The relative changes (%) were obtained by dividing absolute changes by total particle numbers in each size channel. Particle size distributions at 0% RH/100 kPa (open circles) are also presented for the purpose of comparison. Only statistically significant values are plotted (p < 0.05). Error bars represent 95% confidence intervals. Data are from the funnel system using hydrophobic TiO2.
![Figure 5. Changes in particle numbers (%) in individual size channels (measured by SMPS) by increasing 1% relative humidity (left) and by increasing 1 kPa pressure drop (right). The relative changes (%) were obtained by dividing absolute changes by total particle numbers in each size channel. Particle size distributions at 0% RH/100 kPa (open circles) are also presented for the purpose of comparison. Only statistically significant values are plotted (p < 0.05). Error bars represent 95% confidence intervals. Data are from the funnel system using hydrophobic TiO2.](/cms/asset/a7f7f59e-ae6a-478f-a818-512b14cf7dfb/uast_a_1216072_f0005_oc.gif)