Figures & data
Table 1. Representative cylindrical DMAs for classifying large particles.
Figure 2. Experimental schematics for the evaluation of the toroidal Hy-DMA (a) using a TSI standard long-DMA and CPC for sizing accuracy and (b) using two identical Hy-DMAs to obtain the transfer functions of the toroidal Hy-DMA.
![Figure 2. Experimental schematics for the evaluation of the toroidal Hy-DMA (a) using a TSI standard long-DMA and CPC for sizing accuracy and (b) using two identical Hy-DMAs to obtain the transfer functions of the toroidal Hy-DMA.](/cms/asset/ca0f8961-26c2-462b-a6c3-a852218b2419/uast_a_1701625_f0002_c.jpg)
Figure 3. Calculation domain for the numerical study of the toroidal Hy-DMA and the boundary conditions.
![Figure 3. Calculation domain for the numerical study of the toroidal Hy-DMA and the boundary conditions.](/cms/asset/c14b5e1b-fdfb-401e-8b59-739c1c818492/uast_a_1701625_f0003_c.jpg)
Figure 4. (a) Normalized velocity magnitude at the injection line in the aerosol inlet and (b) schematic explanation of the single particle tracking method.
![Figure 4. (a) Normalized velocity magnitude at the injection line in the aerosol inlet and (b) schematic explanation of the single particle tracking method.](/cms/asset/46eec4cb-f12e-4517-ab9a-3ca0db4ee4ea/uast_a_1701625_f0004_c.jpg)
Figure 5. Central electrical mobility as a function of voltage applied to the toroidal Hy-DMA for the sheath-to-aerosol flow rate ratio of 3:0.3 and 5:0.5 L/min.
![Figure 5. Central electrical mobility as a function of voltage applied to the toroidal Hy-DMA for the sheath-to-aerosol flow rate ratio of 3:0.3 and 5:0.5 L/min.](/cms/asset/29c3cd58-00cc-4625-9d47-bcd75ec632ed/uast_a_1701625_f0005_b.jpg)
Figure 6. (a) Comparison between experimental and predicted TDMA curves for the toroidal Hy-DMA for 68 nm particles and (b) transfer functions of the toroidal Hy-DMA for 23, 68, and 238 nm particle sizes obtained via the deconvolution process at the sheath-to-aerosol flow rate ratio of 3:0.3 L/min.
![Figure 6. (a) Comparison between experimental and predicted TDMA curves for the toroidal Hy-DMA for 68 nm particles and (b) transfer functions of the toroidal Hy-DMA for 23, 68, and 238 nm particle sizes obtained via the deconvolution process at the sheath-to-aerosol flow rate ratio of 3:0.3 L/min.](/cms/asset/c2671ff6-f2bf-48bd-a966-ead0af2c0dea/uast_a_1701625_f0006_c.jpg)
Figure 7. Schematic diagram of (a) velocity streamline and (b) vectors of electric field colored by electric potential at the aerosol inlet and monodisperse outlet. The units are [m/s] for the velocity streamline and [V] for the electric potential.
![Figure 7. Schematic diagram of (a) velocity streamline and (b) vectors of electric field colored by electric potential at the aerosol inlet and monodisperse outlet. The units are [m/s] for the velocity streamline and [V] for the electric potential.](/cms/asset/f5419d94-94cb-47dc-9e3c-bae3b32969d8/uast_a_1701625_f0007_c.jpg)
Figure 8. Exemplary particle trajectories of different-sized particles in the toroidal Hy-DMA under the voltage of 320 V and sheath-to-aerosol flow rate ratio of 3:0.3 L/min: (a) 90 nm; (b) 94 nm; (c) 98 nm; (d) 102 nm; (e) 106 nm.
![Figure 8. Exemplary particle trajectories of different-sized particles in the toroidal Hy-DMA under the voltage of 320 V and sheath-to-aerosol flow rate ratio of 3:0.3 L/min: (a) 90 nm; (b) 94 nm; (c) 98 nm; (d) 102 nm; (e) 106 nm.](/cms/asset/6f3bb18c-beb6-478c-b420-3f54336c40ce/uast_a_1701625_f0008_c.jpg)
Figure 9. Transmission probabilities of the toroidal Hy-DMA as a function of particle diameter obtained by the single particle tracking analysis for the sheath-to-aerosol flow rate ratio of (a) 3:0.3 and (b) 5:0.5 L/min.
![Figure 9. Transmission probabilities of the toroidal Hy-DMA as a function of particle diameter obtained by the single particle tracking analysis for the sheath-to-aerosol flow rate ratio of (a) 3:0.3 and (b) 5:0.5 L/min.](/cms/asset/89502238-7c88-417b-a6d5-f033c750a609/uast_a_1701625_f0009_c.jpg)
Table 2. Comparison of central particle sizes obtained by experiments and numerical simulations.
Figure 10. Normalized transmission probabilities as a function of normalized particle electrical mobility obtained by the single particle tracking analysis for the sheath-to-aerosol flow rate ratio of (a) 3:0.3 and (b) 5:0.5 L/min.
![Figure 10. Normalized transmission probabilities as a function of normalized particle electrical mobility obtained by the single particle tracking analysis for the sheath-to-aerosol flow rate ratio of (a) 3:0.3 and (b) 5:0.5 L/min.](/cms/asset/6a0e5274-52ee-4f8e-b8d5-e9f5212c424a/uast_a_1701625_f0010_c.jpg)
Figure 11. (a) Heights and (b) FWHMs, (c) area and (d) sizing resolution of the toroidal Hy-DMA transfer function plotted with those of different types of DMAs from other literatures.
![Figure 11. (a) Heights and (b) FWHMs, (c) area and (d) sizing resolution of the toroidal Hy-DMA transfer function plotted with those of different types of DMAs from other literatures.](/cms/asset/cf5c14e2-5df6-4916-b54e-58c10a7e4249/uast_a_1701625_f0011_c.jpg)