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Original Articles

Effect of Aerosol Volatility on the Sizing Accuracy of Differential Mobility Analyzers

Pages 604-619 | Received 07 Apr 2013, Accepted 15 Feb 2014, Published online: 19 May 2014

Figures & data

Figure 1 Trajectories of stable and volatile (evaporating) particles inside a DMA. Virtual entrance and exit slits for the aerosol and monodisperse flows are represented by short dotted lines near the top and the bottom of each graph.
Figure 1 Trajectories of stable and volatile (evaporating) particles inside a DMA. Virtual entrance and exit slits for the aerosol and monodisperse flows are represented by short dotted lines near the top and the bottom of each graph.
Figure 2 Diagram of the TDMA setup.
Figure 2 Diagram of the TDMA setup.
Figure 3 A comparison of ratios of sampled size to reported nominal size calculated with the simplified and the trajectory models for a compound with Cs = 10 μg/m3. The trajectory model results for the scanning mode with 30 s and 300 s scan rates are also shown.
Figure 3 A comparison of ratios of sampled size to reported nominal size calculated with the simplified and the trajectory models for a compound with Cs = 10 μg/m3. The trajectory model results for the scanning mode with 30 s and 300 s scan rates are also shown.
Figure 4 A compilation of size distributions of aerosol transmitted by the first DMA as measured by the second DMA at 25°C.
Figure 4 A compilation of size distributions of aerosol transmitted by the first DMA as measured by the second DMA at 25°C.

Table 1 Summary of measured midpoint sizes of ammonium sulfate (AS) and ammonium nitrate (AN) aerosol during different experiments. All sizes are in nm

Figure 5 A comparison of observations with the model. Markers indicate the ratio of the measured nominal midpoint size to the nominal size set by the first DMA.
Figure 5 A comparison of observations with the model. Markers indicate the ratio of the measured nominal midpoint size to the nominal size set by the first DMA.
Figure 6 Predicted ratio of nominal diameter (dp, n) to sampled diameter (dp, s) when measuring aerosols of different volatilities at sheath flow 3 L/min.
Figure 6 Predicted ratio of nominal diameter (dp, n) to sampled diameter (dp, s) when measuring aerosols of different volatilities at sheath flow 3 L/min.
Figure 7 Predicted ratio of nominal diameter (dp, n) to sampled diameter (dp, s) at different sheath flow rates.
Figure 7 Predicted ratio of nominal diameter (dp, n) to sampled diameter (dp, s) at different sheath flow rates.
Figure 8 Predicted ratio of transferred diameter (dp, t) to nominal diameter (dp, n) at different sheath flow rates.
Figure 8 Predicted ratio of transferred diameter (dp, t) to nominal diameter (dp, n) at different sheath flow rates.
Figure 9 Predicted ratio of transmitted (Vp, t) to nominal aerosol volume (Vp, n) when measuring ammonium nitrate aerosol at different temperatures using TSI long DMA at 3 L/min sheath flow rate.
Figure 9 Predicted ratio of transmitted (Vp, t) to nominal aerosol volume (Vp, n) when measuring ammonium nitrate aerosol at different temperatures using TSI long DMA at 3 L/min sheath flow rate.

Table 2 Estimated ratio of the transmitted to set mass when selecting 300 nm ammonium nitrate aerosol using a single DMA

Figure 10 Predicted deq, 1/dp, n ratio for ammonium sulfate aerosol assuming different values of water accommodation coefficients (α). Aerosol is initially in metastable equilibrium with air sample at 40% RH. Sheath air RH is 90%.
Figure 10 Predicted deq, 1/dp, n ratio for ammonium sulfate aerosol assuming different values of water accommodation coefficients (α). Aerosol is initially in metastable equilibrium with air sample at 40% RH. Sheath air RH is 90%.
Figure 11 Predicted deq, 1/dp, t ratio for ammonium sulfate aerosol assuming different values of water accommodation coefficients (α). Conditions were taken as in .
Figure 11 Predicted deq, 1/dp, t ratio for ammonium sulfate aerosol assuming different values of water accommodation coefficients (α). Conditions were taken as in Figure 10.
Figure 12 Selection (Ωs) and transfer (Ωt) functions modeled for constant voltage mode of operation when sampling ammonium nitrate aerosol at 3 L/min sheath flow rate. Ωs and Ωt are given for different centroid dp, n of ammonium nitrate, which are indicated above individual functions. The transfer function for a stable aerosol is also given for reference.
Figure 12 Selection (Ωs) and transfer (Ωt) functions modeled for constant voltage mode of operation when sampling ammonium nitrate aerosol at 3 L/min sheath flow rate. Ωs and Ωt are given for different centroid dp, n of ammonium nitrate, which are indicated above individual functions. The transfer function for a stable aerosol is also given for reference.
Figure 13 Selection (Ωs) functions modeled for scanning mode of operation when sampling ammonium nitrate aerosol at 3 L/min sheath flow rate. Ωs are given for different centroid dp, n of ammonium nitrate, which are indicated above individual functions. The selection function for a stable aerosol is also given for reference.
Figure 13 Selection (Ωs) functions modeled for scanning mode of operation when sampling ammonium nitrate aerosol at 3 L/min sheath flow rate. Ωs are given for different centroid dp, n of ammonium nitrate, which are indicated above individual functions. The selection function for a stable aerosol is also given for reference.
Figure 14 Modeled approximation of concentration bias, Rc, when measuring an evaporating aerosol as a function of centroid nominal diameter . Calculations were made for a sheath airflow rate of 3 L/min and scan times of 30 s and 300 s scan times.
Figure 14 Modeled approximation of concentration bias, Rc, when measuring an evaporating aerosol as a function of centroid nominal diameter . Calculations were made for a sheath airflow rate of 3 L/min and scan times of 30 s and 300 s scan times.
Supplemental material

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