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Original Articles

Mobility distributions of Sub 5 nm singly self-charged water soluble and non-soluble particles from a heated NiCr wire in clean dry air

Pages 859-868 | Received 13 Feb 2022, Accepted 21 Jun 2022, Published online: 13 Jul 2022

Figures & data

Figure 1. Experimental set up.

Figure 1. Experimental set up.

Figure 2. Views of the wire at different unknown temperatures.

Figure 2. Views of the wire at different unknown temperatures.

Figure 3. Effect of the temperature on the size distributions of positive singly self-charged particles generated by a heated wire (0.5 mm diameter) in 6 lpm air flowrate.

Figure 3. Effect of the temperature on the size distributions of positive singly self-charged particles generated by a heated wire (0.5 mm diameter) in 6 lpm air flowrate.

Figure 4. Effect of the temperature on the size distributions of negative singly self-charged particles generated by a heated wire (0.5 mm diameter) in 25 lpm air flowrate.

Figure 4. Effect of the temperature on the size distributions of negative singly self-charged particles generated by a heated wire (0.5 mm diameter) in 25 lpm air flowrate.

Figure 5. Views of the deposited salt on the thick electrodes of the high current feedthrough of the cross.

Figure 5. Views of the deposited salt on the thick electrodes of the high current feedthrough of the cross.

Figure 6. Positive and negative sodium chloride (NaCl+ and NaCl-) size distributions particles at two different temperatures and air flowrate.

Figure 6. Positive and negative sodium chloride (NaCl+ and NaCl-) size distributions particles at two different temperatures and air flowrate.

Figure 7. Positive and negative sodium chloride (KCl) size distributions particles at two different temperatures and air flowrates.

Figure 7. Positive and negative sodium chloride (KCl) size distributions particles at two different temperatures and air flowrates.

Figure 8. Effect of the voltage bias of the wire against the grounded cross body on the size distributions and total concentrations.

Figure 8. Effect of the voltage bias of the wire against the grounded cross body on the size distributions and total concentrations.

Figure 9. Evolution of the concentration of particles over the time for 3 different diameters in the sub 3 nm range.

Figure 9. Evolution of the concentration of particles over the time for 3 different diameters in the sub 3 nm range.

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