Figures & data
FIG. 1 (a) Tube with length L and radius R where L ≫ R, and with grids on both ends, (b) tube with L ≫ R, (c) ring with L ≪ R, and (d) the tube of (b) split into two equal segments.
![FIG. 1 (a) Tube with length L and radius R where L ≫ R, and with grids on both ends, (b) tube with L ≫ R, (c) ring with L ≪ R, and (d) the tube of (b) split into two equal segments.](/cms/asset/d3dd9bf7-4631-4315-9691-1c85c78bb344/uast_a_875981_o_f0001g.gif)
FIG. 2 Scheme of our new instrument. Similar previous instruments use a filter to capture the particles in a Faraday cup electrometer, whereas we use an open Faraday cage.
![FIG. 2 Scheme of our new instrument. Similar previous instruments use a filter to capture the particles in a Faraday cup electrometer, whereas we use an open Faraday cage.](/cms/asset/9fcbef2c-6e43-4df1-a7dd-116b0af0b565/uast_a_875981_o_f0002g.gif)
FIG. 4 Electrometer signal with 50 nm NaCl particles of a concentration of 1.7*104 pt/ccm (gray) and charging current (black) for different pulse settings.
![FIG. 4 Electrometer signal with 50 nm NaCl particles of a concentration of 1.7*104 pt/ccm (gray) and charging current (black) for different pulse settings.](/cms/asset/5e48ba2f-6fe8-4f11-8c93-04f3727b8791/uast_a_875981_o_f0004g.gif)
FIG. 5 Determination of lower detection limit with 50 nm NaCl particles. Left: time series of signals measured by CPC and partector for decreasing dilution. Right: averaged values over each concentration step. The line is a guide to the eye. The partector signal deviates from the 1:1 line for low concentrations due to instrument noise.
![FIG. 5 Determination of lower detection limit with 50 nm NaCl particles. Left: time series of signals measured by CPC and partector for decreasing dilution. Right: averaged values over each concentration step. The line is a guide to the eye. The partector signal deviates from the 1:1 line for low concentrations due to instrument noise.](/cms/asset/8ab4ccbb-a02f-41f7-a164-914a29b62ffd/uast_a_875981_o_f0005g.gif)