1959
DOI: 10.1016/0009-2509(59)80061-0
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The deposition of airborne droplets on wire gauzes

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Cited by 5 publications
(3 citation statements)
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“…The collection efficiency by inertial impaction, E I , is calculated for potential flow and the comparisons are shown in Figure 7a. When aerosol inertia is negligible, similar computations for both viscous and potential flows are performed to estimate the interception efficiency E R and the results are also compared with the previous theoretical studies (Ranz and Wong 1952;Fuchs 1964;Friedlander 1957), with the results shown in Figure 7b, where the interception parameter is defined as Figure 7a indicates that when inertial impaction is the dominant mechanism for aerosol collection, the efficiency curve of the present calculation agrees well with the test data by the previous studies (Ranz and Wong 1952;Jarman 1959;Walton and Woolcock 1960;Schmidt and L€ offler 1993), while the predicted curve obtained by Slinn's formula (Slinn 1983;Seinfeld and Pandis 2006) underestimates the inertial collection efficiency. Figure 7b shows that the calculations of interception efficiencies in this study, for both the viscous and the potential flows, are in good agreement with those of theoretical predictions (Fuchs 1964;Friedlander 1957;Ranz and Wong 1952).…”
Section: Validations Of Computational Methodssupporting
confidence: 82%
See 1 more Smart Citation
“…The collection efficiency by inertial impaction, E I , is calculated for potential flow and the comparisons are shown in Figure 7a. When aerosol inertia is negligible, similar computations for both viscous and potential flows are performed to estimate the interception efficiency E R and the results are also compared with the previous theoretical studies (Ranz and Wong 1952;Fuchs 1964;Friedlander 1957), with the results shown in Figure 7b, where the interception parameter is defined as Figure 7a indicates that when inertial impaction is the dominant mechanism for aerosol collection, the efficiency curve of the present calculation agrees well with the test data by the previous studies (Ranz and Wong 1952;Jarman 1959;Walton and Woolcock 1960;Schmidt and L€ offler 1993), while the predicted curve obtained by Slinn's formula (Slinn 1983;Seinfeld and Pandis 2006) underestimates the inertial collection efficiency. Figure 7b shows that the calculations of interception efficiencies in this study, for both the viscous and the potential flows, are in good agreement with those of theoretical predictions (Fuchs 1964;Friedlander 1957;Ranz and Wong 1952).…”
Section: Validations Of Computational Methodssupporting
confidence: 82%
“…Numerous studies have been conducted to investigate the capture of particles on spherical collectors by the mechanisms of inertial impaction and interception (Ranz and Wong 1952;Jarman 1959;Walton and Woolcock 1960;Schmidt and L€ offler 1993;Fuchs 1964;Friedlander 1957;Slinn 1983). The numerical model used in this study is validated against the results mentioned above, including experimental data and theoretical predictions, and the results are shown in Figure 7.…”
Section: Validations Of Computational Methodsmentioning
confidence: 99%
“…This is probably mainly due to the different aerodynamic assumptions made. By comparing equations (10) and (11) it can be shown that n = 0 is more critical than rc^O unless 12 ( 1 -v 2 ) (I)" (12) For a shell with a /h = 400 this implies n^3 6 and for this number of circumferential waves the circumferential mode is essentially circular anyway.…”
Section: -{(R)'[»•-"-]-(t)"["•-»-]}'mentioning
confidence: 99%