@article{
 title = {Numerical characterization of particle beam collimation: Part II - Integrated aerodynamic-lens-nozzle system},
 type = {article},
 year = {2004},
 identifiers = {[object Object]},
 keywords = {controlled dimensions,divergence,expansions,mass-spectrometer,motion},
 pages = {619-638},
 volume = {38},
 websites = {<Go to ISI>://000222953800006},
 id = {44b1699b-5bc8-3d82-b9d8-d5edaee38b3c},
 created = {2015-02-12T14:35:24.000Z},
 file_attached = {true},
 profile_id = {63309e83-e060-32e4-b606-af50e203809b},
 group_id = {63e349d6-2c70-3938-9e67-2f6483f6cbab},
 last_modified = {2015-06-12T17:36:27.000Z},
 read = {false},
 starred = {false},
 authored = {false},
 confirmed = {true},
 hidden = {false},
 source_type = {Journal Article},
 language = {English},
 notes = {
        <m:bold>From Duplicate 1 ( </m:bold>
        <m:bold>
          <m:italic>Numerical characterization of particle beam collimation: Part II - Integrated aerodynamic-lens-nozzle system</m:italic>
        </m:bold>
        <m:bold> - Zhang, X F; Smith, K A; Worsnop, D R; Jimenez, J L; Jayne, J T; Kolb, C E; Morris, J; Davidovits, P )<m:linebreak></m:linebreak>
        </m:bold>
        <m:linebreak></m:linebreak>841TF<m:linebreak></m:linebreak>Times Cited:0<m:linebreak></m:linebreak>Cited References Count:6<m:linebreak></m:linebreak>
        <m:linebreak></m:linebreak>
      },
 abstract = {As a sequel to our previous effort on the modeling of particle motion through a single lens or nozzle, flows of gas-particle suspensions through an integrated aerodynamic-lens-nozzle inlet have been investigated numerically. It is found that the inlet transmission efficiency (eta(t)) is unity for particles of intermediate diameters (D-p similar to30-500 nm). The transmission efficiency gradually diminishes to similar to40% for large particles (D-p > 2500 nm) because of impact losses on the surface of the first lens. There is a catastrophic reduction of eta(t) to almost zero for very small particles (D-p less than or equal to 15 nm) because these particles faithfully follow the final gas expansion. We found that, for very small particles, particle transmission is mainly controlled by nozzle geometry and operating conditions. A lower upstream pressure or a small inlet can be used to improve transmission of very small particles, but at the expense of sampling rate, or vice versa. Brownian motion exacerbates the catastrophic reduction in eta(t) for small particles; we found that the overall particle transmission efficiency can be roughly calculated as the product of the aerodynamic and the purely Brownian efficiencies. For particles of intermediate diameters, Brownian motion is irrelevant, and the modeling results show that the transmission efficiency is mainly controlled by the lenses. Results for an isolated lens or nozzle are used to provide guidance for the design of alternative inlets. Several examples are given, in which it is shown that one can configure the inlet to preferentially sample large particles (with eta(t) > 50% for D-p = 50-2000 nm) or ultrafine particles (with eta(t) > 50% for D-p = 20-1000 nm). Some of the results have been compared with experimental data, and reasonable agreement has been demonstrated.},
 bibtype = {article},
 author = {Zhang, X F and Smith, K A and Worsnop, D R and Jimenez, J L and Jayne, J T and Kolb, C E and Morris, J W and Davidovits, P},
 journal = {Aerosol Science and Technology},
 number = {6}
}

{"_id":"xxcWnLzQ8eCmLLd5D","bibbaseid":"zhang-smith-worsnop-jimenez-jayne-kolb-morris-davidovits-numericalcharacterizationofparticlebeamcollimationpartiiintegratedaerodynamiclensnozzlesystem-2004","downloads":0,"creationDate":"2017-01-12T21:32:11.809Z","title":"Numerical characterization of particle beam collimation: Part II - Integrated aerodynamic-lens-nozzle system","author_short":["Zhang, X., F.","Smith, K., A.","Worsnop, D., R.","Jimenez, J., L.","Jayne, J., T.","Kolb, C., E.","Morris, J., W.","Davidovits, P."],"year":2004,"bibtype":"article","biburl":null,"bibdata":{"title":"Numerical characterization of particle beam collimation: Part II - Integrated aerodynamic-lens-nozzle system","type":"article","year":"2004","identifiers":"[object Object]","keywords":"controlled dimensions,divergence,expansions,mass-spectrometer,motion","pages":"619-638","volume":"38","websites":"<Go to ISI>://000222953800006","id":"44b1699b-5bc8-3d82-b9d8-d5edaee38b3c","created":"2015-02-12T14:35:24.000Z","file_attached":"true","profile_id":"63309e83-e060-32e4-b606-af50e203809b","group_id":"63e349d6-2c70-3938-9e67-2f6483f6cbab","last_modified":"2015-06-12T17:36:27.000Z","read":false,"starred":false,"authored":false,"confirmed":"true","hidden":false,"source_type":"Journal Article","language":"English","notes":"\n <m:bold>From Duplicate 1 ( </m:bold>\n <m:bold>\n <m:italic>Numerical characterization of particle beam collimation: Part II - Integrated aerodynamic-lens-nozzle system</m:italic>\n </m:bold>\n <m:bold> - Zhang, X F; Smith, K A; Worsnop, D R; Jimenez, J L; Jayne, J T; Kolb, C E; Morris, J; Davidovits, P )<m:linebreak></m:linebreak>\n </m:bold>\n <m:linebreak></m:linebreak>841TF<m:linebreak></m:linebreak>Times Cited:0<m:linebreak></m:linebreak>Cited References Count:6<m:linebreak></m:linebreak>\n <m:linebreak></m:linebreak>\n ","abstract":"As a sequel to our previous effort on the modeling of particle motion through a single lens or nozzle, flows of gas-particle suspensions through an integrated aerodynamic-lens-nozzle inlet have been investigated numerically. It is found that the inlet transmission efficiency (eta(t)) is unity for particles of intermediate diameters (D-p similar to30-500 nm). The transmission efficiency gradually diminishes to similar to40% for large particles (D-p > 2500 nm) because of impact losses on the surface of the first lens. There is a catastrophic reduction of eta(t) to almost zero for very small particles (D-p less than or equal to 15 nm) because these particles faithfully follow the final gas expansion. We found that, for very small particles, particle transmission is mainly controlled by nozzle geometry and operating conditions. A lower upstream pressure or a small inlet can be used to improve transmission of very small particles, but at the expense of sampling rate, or vice versa. Brownian motion exacerbates the catastrophic reduction in eta(t) for small particles; we found that the overall particle transmission efficiency can be roughly calculated as the product of the aerodynamic and the purely Brownian efficiencies. For particles of intermediate diameters, Brownian motion is irrelevant, and the modeling results show that the transmission efficiency is mainly controlled by the lenses. Results for an isolated lens or nozzle are used to provide guidance for the design of alternative inlets. Several examples are given, in which it is shown that one can configure the inlet to preferentially sample large particles (with eta(t) > 50% for D-p = 50-2000 nm) or ultrafine particles (with eta(t) > 50% for D-p = 20-1000 nm). Some of the results have been compared with experimental data, and reasonable agreement has been demonstrated.","bibtype":"article","author":"Zhang, X F and Smith, K A and Worsnop, D R and Jimenez, J L and Jayne, J T and Kolb, C E and Morris, J W and Davidovits, P","journal":"Aerosol Science and Technology","number":"6","bibtex":"@article{\n title = {Numerical characterization of particle beam collimation: Part II - Integrated aerodynamic-lens-nozzle system},\n type = {article},\n year = {2004},\n identifiers = {[object Object]},\n keywords = {controlled dimensions,divergence,expansions,mass-spectrometer,motion},\n pages = {619-638},\n volume = {38},\n websites = {<Go to ISI>://000222953800006},\n id = {44b1699b-5bc8-3d82-b9d8-d5edaee38b3c},\n created = {2015-02-12T14:35:24.000Z},\n file_attached = {true},\n profile_id = {63309e83-e060-32e4-b606-af50e203809b},\n group_id = {63e349d6-2c70-3938-9e67-2f6483f6cbab},\n last_modified = {2015-06-12T17:36:27.000Z},\n read = {false},\n starred = {false},\n authored = {false},\n confirmed = {true},\n hidden = {false},\n source_type = {Journal Article},\n language = {English},\n notes = {\n <m:bold>From Duplicate 1 ( </m:bold>\n <m:bold>\n <m:italic>Numerical characterization of particle beam collimation: Part II - Integrated aerodynamic-lens-nozzle system</m:italic>\n </m:bold>\n <m:bold> - Zhang, X F; Smith, K A; Worsnop, D R; Jimenez, J L; Jayne, J T; Kolb, C E; Morris, J; Davidovits, P )<m:linebreak></m:linebreak>\n </m:bold>\n <m:linebreak></m:linebreak>841TF<m:linebreak></m:linebreak>Times Cited:0<m:linebreak></m:linebreak>Cited References Count:6<m:linebreak></m:linebreak>\n <m:linebreak></m:linebreak>\n },\n abstract = {As a sequel to our previous effort on the modeling of particle motion through a single lens or nozzle, flows of gas-particle suspensions through an integrated aerodynamic-lens-nozzle inlet have been investigated numerically. It is found that the inlet transmission efficiency (eta(t)) is unity for particles of intermediate diameters (D-p similar to30-500 nm). The transmission efficiency gradually diminishes to similar to40% for large particles (D-p > 2500 nm) because of impact losses on the surface of the first lens. There is a catastrophic reduction of eta(t) to almost zero for very small particles (D-p less than or equal to 15 nm) because these particles faithfully follow the final gas expansion. We found that, for very small particles, particle transmission is mainly controlled by nozzle geometry and operating conditions. A lower upstream pressure or a small inlet can be used to improve transmission of very small particles, but at the expense of sampling rate, or vice versa. Brownian motion exacerbates the catastrophic reduction in eta(t) for small particles; we found that the overall particle transmission efficiency can be roughly calculated as the product of the aerodynamic and the purely Brownian efficiencies. For particles of intermediate diameters, Brownian motion is irrelevant, and the modeling results show that the transmission efficiency is mainly controlled by the lenses. Results for an isolated lens or nozzle are used to provide guidance for the design of alternative inlets. Several examples are given, in which it is shown that one can configure the inlet to preferentially sample large particles (with eta(t) > 50% for D-p = 50-2000 nm) or ultrafine particles (with eta(t) > 50% for D-p = 20-1000 nm). Some of the results have been compared with experimental data, and reasonable agreement has been demonstrated.},\n bibtype = {article},\n author = {Zhang, X F and Smith, K A and Worsnop, D R and Jimenez, J L and Jayne, J T and Kolb, C E and Morris, J W and Davidovits, P},\n journal = {Aerosol Science and Technology},\n number = {6}\n}","author_short":["Zhang, X., F.","Smith, K., A.","Worsnop, D., R.","Jimenez, J., L.","Jayne, J., T.","Kolb, C., E.","Morris, J., W.","Davidovits, P."],"urls":{"Paper":"http://bibbase.org/service/mendeley/9edae5ec-3a23-3830-8934-2c27bef6ccbe/file/3ef148d5-3890-ad4f-6532-baa351a441a0/2004-Numerical_characterization_of_particle_beam_collimation_Part_II_-_Integrated_aerodynamic-lens-nozzle_system.pdf.pdf","Website":"<Go to ISI>://000222953800006"},"bibbaseid":"zhang-smith-worsnop-jimenez-jayne-kolb-morris-davidovits-numericalcharacterizationofparticlebeamcollimationpartiiintegratedaerodynamiclensnozzlesystem-2004","role":"author","keyword":["controlled dimensions","divergence","expansions","mass-spectrometer","motion"],"downloads":0},"search_terms":["numerical","characterization","particle","beam","collimation","part","integrated","aerodynamic","lens","nozzle","system","zhang","smith","worsnop","jimenez","jayne","kolb","morris","davidovits"],"keywords":["controlled dimensions","divergence","expansions","mass-spectrometer","motion"],"authorIDs":[]}