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The resulting change in the electrical mobility distribution and the number of charge are measured by the aerosol measurement techniques.
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A scanning mobility particle sizer (SMPS), combining a differential mobility analyzer (DMA, 4220, HCT Co., Ltd, Icheon, Korea) and condensation particle counter (CPC, 4312, HCT Co., Ltd), was used to monitor the particle size distribution with an electrical mobility diameter ranging from 7.37 to 289.03 nm.
An SMPS combining a differential mobility analyzer (DMA, 4220, HCT Co., Ltd., Korea) and condensation particle counter (CPC, 4312, HCT Co., Ltd., 0 10 particles/cm detection range) was used to monitor the particle size distribution with an electrical mobility diameter ranging from 15 to 710.5 nm.
This paper presents a new design for a multi-channel electrical mobility spectrometer which measures the lognormal size distribution and number concentration of aerosol particles in the size range 5 300 nm with a short response time.
For an electrical mobility analyzer, the charging is aimed to impose a known net charge distribution on each aerosol size.
Particle size distribution and number concentration were monitored continuously by a differential electrical mobility particle sizer and a condensation particle counter.
Recently, nanoparticles have been studied more extensively by real-time size-resolved particle distributions for instance by electrical low-pressure impactor and differential electrical mobility particle spectrometry [ 8, 12, 13, 14].
Electrical mobility measurements of the soot particles generated in rich premixed ethylene/air flat flames reveal a characteristic lognormal size distribution that is distinct from the self preserving distribution expected from coagulation dominated aerosol dynamics.
The particle size distributions in dried samples of the inhaled and exhaled air are characterised with an electrical mobility spectrometer.
The gas conductivity depends on charge density and electrical mobility of the charges.
Assume the traffic mobility distribution is the same as [22].
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