Evaluation of the Performance in Charging Efficiencies and Losses of Ultrafine Particles Ranging in Sizes from 15 to 75 nm in a Unipolar Corona-based Ionizer
Abstract For this study, a unipolar corona-based ionizer was constructed and experimentally evaluated for charging efficiencies and losses of ultrafine particles in the size range of 15–75 nm at different corona voltage, ion trap voltage and particle flow rate. The corona voltage was applied to the...
Ausführliche Beschreibung
Autor*in: |
Intra, Panich [verfasserIn] Wanusbodeepaisarn, Paisarn [verfasserIn] Siri-achawawath, Thanesvorn [verfasserIn] |
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Format: |
E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2020 |
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Schlagwörter: |
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Übergeordnetes Werk: |
Enthalten in: Journal of electrical engineering & technology - [Singapore] : Springer Singapore, 2006, 16(2020), 2 vom: 14. Dez., Seite 963-974 |
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Übergeordnetes Werk: |
volume:16 ; year:2020 ; number:2 ; day:14 ; month:12 ; pages:963-974 |
Links: |
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DOI / URN: |
10.1007/s42835-020-00623-2 |
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Katalog-ID: |
SPR043373550 |
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520 | |a Abstract For this study, a unipolar corona-based ionizer was constructed and experimentally evaluated for charging efficiencies and losses of ultrafine particles in the size range of 15–75 nm at different corona voltage, ion trap voltage and particle flow rate. The corona voltage was applied to the ionizer between 2.0–3.0 kV. The discharge currents increased from 0.16 nA to 4.23 μA and the ion number concentration increased from 6.27 × $ 10^{9} $ to 1.36 × $ 10^{14} $ ions/$ m^{3} $. Increasing the corona voltage lead to a higher discharge current and ion number concentration in the ionizer. The best intrinsic charging efficiency of the ionizer was about 92.15–99.33% for particle diameters ranging from 15 to 75 nm, and occurred at corona voltage, ion trap voltage and particle flow rate of about 3.0 kV, 100 V, 0.6 L/min, respectively. At a given corona voltage, the extrinsic charging efficiency increased as the particle flow rate increased. The best extrinsic charging efficiency ranged from 14.93 to 57.70% for particle diameters increasing from 15 to 75 nm, and occurred at corona voltage, ion trap voltage and particle flow rate of about 2.6 kV, 100 V, and 1.5 L/min, respectively. In the present ionizer, the highest electrostatic loss was observed for particles with a diameter of about 45 nm, and it was about 88.03% at a corona voltage of 3.0 kV and an ion trap voltage of 200 V. Finally, the highest diffusion loss of about 22.66% was seen to occur with singly charged particles with a diameter of 15 nm at the particle flow rate of about 0.6 L/min. | ||
650 | 4 | |a Corona discharge |7 (dpeaa)DE-He213 | |
650 | 4 | |a Particle charging |7 (dpeaa)DE-He213 | |
650 | 4 | |a Particle ionizer |7 (dpeaa)DE-He213 | |
650 | 4 | |a Particle loss |7 (dpeaa)DE-He213 | |
650 | 4 | |a Charging efficiency |7 (dpeaa)DE-He213 | |
700 | 1 | |a Wanusbodeepaisarn, Paisarn |e verfasserin |4 aut | |
700 | 1 | |a Siri-achawawath, Thanesvorn |e verfasserin |4 aut | |
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10.1007/s42835-020-00623-2 doi (DE-627)SPR043373550 (DE-599)SPRs42835-020-00623-2-e (SPR)s42835-020-00623-2-e DE-627 ger DE-627 rakwb eng 620 ASE 620 ASE Intra, Panich verfasserin aut Evaluation of the Performance in Charging Efficiencies and Losses of Ultrafine Particles Ranging in Sizes from 15 to 75 nm in a Unipolar Corona-based Ionizer 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract For this study, a unipolar corona-based ionizer was constructed and experimentally evaluated for charging efficiencies and losses of ultrafine particles in the size range of 15–75 nm at different corona voltage, ion trap voltage and particle flow rate. The corona voltage was applied to the ionizer between 2.0–3.0 kV. The discharge currents increased from 0.16 nA to 4.23 μA and the ion number concentration increased from 6.27 × $ 10^{9} $ to 1.36 × $ 10^{14} $ ions/$ m^{3} $. Increasing the corona voltage lead to a higher discharge current and ion number concentration in the ionizer. The best intrinsic charging efficiency of the ionizer was about 92.15–99.33% for particle diameters ranging from 15 to 75 nm, and occurred at corona voltage, ion trap voltage and particle flow rate of about 3.0 kV, 100 V, 0.6 L/min, respectively. At a given corona voltage, the extrinsic charging efficiency increased as the particle flow rate increased. The best extrinsic charging efficiency ranged from 14.93 to 57.70% for particle diameters increasing from 15 to 75 nm, and occurred at corona voltage, ion trap voltage and particle flow rate of about 2.6 kV, 100 V, and 1.5 L/min, respectively. In the present ionizer, the highest electrostatic loss was observed for particles with a diameter of about 45 nm, and it was about 88.03% at a corona voltage of 3.0 kV and an ion trap voltage of 200 V. Finally, the highest diffusion loss of about 22.66% was seen to occur with singly charged particles with a diameter of 15 nm at the particle flow rate of about 0.6 L/min. Corona discharge (dpeaa)DE-He213 Particle charging (dpeaa)DE-He213 Particle ionizer (dpeaa)DE-He213 Particle loss (dpeaa)DE-He213 Charging efficiency (dpeaa)DE-He213 Wanusbodeepaisarn, Paisarn verfasserin aut Siri-achawawath, Thanesvorn verfasserin aut Enthalten in Journal of electrical engineering & technology [Singapore] : Springer Singapore, 2006 16(2020), 2 vom: 14. Dez., Seite 963-974 (DE-627)519202015 (DE-600)2255142-6 2093-7423 nnns volume:16 year:2020 number:2 day:14 month:12 pages:963-974 https://dx.doi.org/10.1007/s42835-020-00623-2 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 16 2020 2 14 12 963-974 |
spelling |
10.1007/s42835-020-00623-2 doi (DE-627)SPR043373550 (DE-599)SPRs42835-020-00623-2-e (SPR)s42835-020-00623-2-e DE-627 ger DE-627 rakwb eng 620 ASE 620 ASE Intra, Panich verfasserin aut Evaluation of the Performance in Charging Efficiencies and Losses of Ultrafine Particles Ranging in Sizes from 15 to 75 nm in a Unipolar Corona-based Ionizer 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract For this study, a unipolar corona-based ionizer was constructed and experimentally evaluated for charging efficiencies and losses of ultrafine particles in the size range of 15–75 nm at different corona voltage, ion trap voltage and particle flow rate. The corona voltage was applied to the ionizer between 2.0–3.0 kV. The discharge currents increased from 0.16 nA to 4.23 μA and the ion number concentration increased from 6.27 × $ 10^{9} $ to 1.36 × $ 10^{14} $ ions/$ m^{3} $. Increasing the corona voltage lead to a higher discharge current and ion number concentration in the ionizer. The best intrinsic charging efficiency of the ionizer was about 92.15–99.33% for particle diameters ranging from 15 to 75 nm, and occurred at corona voltage, ion trap voltage and particle flow rate of about 3.0 kV, 100 V, 0.6 L/min, respectively. At a given corona voltage, the extrinsic charging efficiency increased as the particle flow rate increased. The best extrinsic charging efficiency ranged from 14.93 to 57.70% for particle diameters increasing from 15 to 75 nm, and occurred at corona voltage, ion trap voltage and particle flow rate of about 2.6 kV, 100 V, and 1.5 L/min, respectively. In the present ionizer, the highest electrostatic loss was observed for particles with a diameter of about 45 nm, and it was about 88.03% at a corona voltage of 3.0 kV and an ion trap voltage of 200 V. Finally, the highest diffusion loss of about 22.66% was seen to occur with singly charged particles with a diameter of 15 nm at the particle flow rate of about 0.6 L/min. Corona discharge (dpeaa)DE-He213 Particle charging (dpeaa)DE-He213 Particle ionizer (dpeaa)DE-He213 Particle loss (dpeaa)DE-He213 Charging efficiency (dpeaa)DE-He213 Wanusbodeepaisarn, Paisarn verfasserin aut Siri-achawawath, Thanesvorn verfasserin aut Enthalten in Journal of electrical engineering & technology [Singapore] : Springer Singapore, 2006 16(2020), 2 vom: 14. Dez., Seite 963-974 (DE-627)519202015 (DE-600)2255142-6 2093-7423 nnns volume:16 year:2020 number:2 day:14 month:12 pages:963-974 https://dx.doi.org/10.1007/s42835-020-00623-2 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 16 2020 2 14 12 963-974 |
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10.1007/s42835-020-00623-2 doi (DE-627)SPR043373550 (DE-599)SPRs42835-020-00623-2-e (SPR)s42835-020-00623-2-e DE-627 ger DE-627 rakwb eng 620 ASE 620 ASE Intra, Panich verfasserin aut Evaluation of the Performance in Charging Efficiencies and Losses of Ultrafine Particles Ranging in Sizes from 15 to 75 nm in a Unipolar Corona-based Ionizer 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract For this study, a unipolar corona-based ionizer was constructed and experimentally evaluated for charging efficiencies and losses of ultrafine particles in the size range of 15–75 nm at different corona voltage, ion trap voltage and particle flow rate. The corona voltage was applied to the ionizer between 2.0–3.0 kV. The discharge currents increased from 0.16 nA to 4.23 μA and the ion number concentration increased from 6.27 × $ 10^{9} $ to 1.36 × $ 10^{14} $ ions/$ m^{3} $. Increasing the corona voltage lead to a higher discharge current and ion number concentration in the ionizer. The best intrinsic charging efficiency of the ionizer was about 92.15–99.33% for particle diameters ranging from 15 to 75 nm, and occurred at corona voltage, ion trap voltage and particle flow rate of about 3.0 kV, 100 V, 0.6 L/min, respectively. At a given corona voltage, the extrinsic charging efficiency increased as the particle flow rate increased. The best extrinsic charging efficiency ranged from 14.93 to 57.70% for particle diameters increasing from 15 to 75 nm, and occurred at corona voltage, ion trap voltage and particle flow rate of about 2.6 kV, 100 V, and 1.5 L/min, respectively. In the present ionizer, the highest electrostatic loss was observed for particles with a diameter of about 45 nm, and it was about 88.03% at a corona voltage of 3.0 kV and an ion trap voltage of 200 V. Finally, the highest diffusion loss of about 22.66% was seen to occur with singly charged particles with a diameter of 15 nm at the particle flow rate of about 0.6 L/min. Corona discharge (dpeaa)DE-He213 Particle charging (dpeaa)DE-He213 Particle ionizer (dpeaa)DE-He213 Particle loss (dpeaa)DE-He213 Charging efficiency (dpeaa)DE-He213 Wanusbodeepaisarn, Paisarn verfasserin aut Siri-achawawath, Thanesvorn verfasserin aut Enthalten in Journal of electrical engineering & technology [Singapore] : Springer Singapore, 2006 16(2020), 2 vom: 14. Dez., Seite 963-974 (DE-627)519202015 (DE-600)2255142-6 2093-7423 nnns volume:16 year:2020 number:2 day:14 month:12 pages:963-974 https://dx.doi.org/10.1007/s42835-020-00623-2 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 16 2020 2 14 12 963-974 |
allfieldsGer |
10.1007/s42835-020-00623-2 doi (DE-627)SPR043373550 (DE-599)SPRs42835-020-00623-2-e (SPR)s42835-020-00623-2-e DE-627 ger DE-627 rakwb eng 620 ASE 620 ASE Intra, Panich verfasserin aut Evaluation of the Performance in Charging Efficiencies and Losses of Ultrafine Particles Ranging in Sizes from 15 to 75 nm in a Unipolar Corona-based Ionizer 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract For this study, a unipolar corona-based ionizer was constructed and experimentally evaluated for charging efficiencies and losses of ultrafine particles in the size range of 15–75 nm at different corona voltage, ion trap voltage and particle flow rate. The corona voltage was applied to the ionizer between 2.0–3.0 kV. The discharge currents increased from 0.16 nA to 4.23 μA and the ion number concentration increased from 6.27 × $ 10^{9} $ to 1.36 × $ 10^{14} $ ions/$ m^{3} $. Increasing the corona voltage lead to a higher discharge current and ion number concentration in the ionizer. The best intrinsic charging efficiency of the ionizer was about 92.15–99.33% for particle diameters ranging from 15 to 75 nm, and occurred at corona voltage, ion trap voltage and particle flow rate of about 3.0 kV, 100 V, 0.6 L/min, respectively. At a given corona voltage, the extrinsic charging efficiency increased as the particle flow rate increased. The best extrinsic charging efficiency ranged from 14.93 to 57.70% for particle diameters increasing from 15 to 75 nm, and occurred at corona voltage, ion trap voltage and particle flow rate of about 2.6 kV, 100 V, and 1.5 L/min, respectively. In the present ionizer, the highest electrostatic loss was observed for particles with a diameter of about 45 nm, and it was about 88.03% at a corona voltage of 3.0 kV and an ion trap voltage of 200 V. Finally, the highest diffusion loss of about 22.66% was seen to occur with singly charged particles with a diameter of 15 nm at the particle flow rate of about 0.6 L/min. Corona discharge (dpeaa)DE-He213 Particle charging (dpeaa)DE-He213 Particle ionizer (dpeaa)DE-He213 Particle loss (dpeaa)DE-He213 Charging efficiency (dpeaa)DE-He213 Wanusbodeepaisarn, Paisarn verfasserin aut Siri-achawawath, Thanesvorn verfasserin aut Enthalten in Journal of electrical engineering & technology [Singapore] : Springer Singapore, 2006 16(2020), 2 vom: 14. Dez., Seite 963-974 (DE-627)519202015 (DE-600)2255142-6 2093-7423 nnns volume:16 year:2020 number:2 day:14 month:12 pages:963-974 https://dx.doi.org/10.1007/s42835-020-00623-2 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 16 2020 2 14 12 963-974 |
allfieldsSound |
10.1007/s42835-020-00623-2 doi (DE-627)SPR043373550 (DE-599)SPRs42835-020-00623-2-e (SPR)s42835-020-00623-2-e DE-627 ger DE-627 rakwb eng 620 ASE 620 ASE Intra, Panich verfasserin aut Evaluation of the Performance in Charging Efficiencies and Losses of Ultrafine Particles Ranging in Sizes from 15 to 75 nm in a Unipolar Corona-based Ionizer 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract For this study, a unipolar corona-based ionizer was constructed and experimentally evaluated for charging efficiencies and losses of ultrafine particles in the size range of 15–75 nm at different corona voltage, ion trap voltage and particle flow rate. The corona voltage was applied to the ionizer between 2.0–3.0 kV. The discharge currents increased from 0.16 nA to 4.23 μA and the ion number concentration increased from 6.27 × $ 10^{9} $ to 1.36 × $ 10^{14} $ ions/$ m^{3} $. Increasing the corona voltage lead to a higher discharge current and ion number concentration in the ionizer. The best intrinsic charging efficiency of the ionizer was about 92.15–99.33% for particle diameters ranging from 15 to 75 nm, and occurred at corona voltage, ion trap voltage and particle flow rate of about 3.0 kV, 100 V, 0.6 L/min, respectively. At a given corona voltage, the extrinsic charging efficiency increased as the particle flow rate increased. The best extrinsic charging efficiency ranged from 14.93 to 57.70% for particle diameters increasing from 15 to 75 nm, and occurred at corona voltage, ion trap voltage and particle flow rate of about 2.6 kV, 100 V, and 1.5 L/min, respectively. In the present ionizer, the highest electrostatic loss was observed for particles with a diameter of about 45 nm, and it was about 88.03% at a corona voltage of 3.0 kV and an ion trap voltage of 200 V. Finally, the highest diffusion loss of about 22.66% was seen to occur with singly charged particles with a diameter of 15 nm at the particle flow rate of about 0.6 L/min. Corona discharge (dpeaa)DE-He213 Particle charging (dpeaa)DE-He213 Particle ionizer (dpeaa)DE-He213 Particle loss (dpeaa)DE-He213 Charging efficiency (dpeaa)DE-He213 Wanusbodeepaisarn, Paisarn verfasserin aut Siri-achawawath, Thanesvorn verfasserin aut Enthalten in Journal of electrical engineering & technology [Singapore] : Springer Singapore, 2006 16(2020), 2 vom: 14. Dez., Seite 963-974 (DE-627)519202015 (DE-600)2255142-6 2093-7423 nnns volume:16 year:2020 number:2 day:14 month:12 pages:963-974 https://dx.doi.org/10.1007/s42835-020-00623-2 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 16 2020 2 14 12 963-974 |
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English |
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Enthalten in Journal of electrical engineering & technology 16(2020), 2 vom: 14. Dez., Seite 963-974 volume:16 year:2020 number:2 day:14 month:12 pages:963-974 |
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Corona discharge Particle charging Particle ionizer Particle loss Charging efficiency |
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Journal of electrical engineering & technology |
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Intra, Panich @@aut@@ Wanusbodeepaisarn, Paisarn @@aut@@ Siri-achawawath, Thanesvorn @@aut@@ |
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2020-12-14T00:00:00Z |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">SPR043373550</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20220112044847.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">210302s2020 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s42835-020-00623-2</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR043373550</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-599)SPRs42835-020-00623-2-e</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s42835-020-00623-2-e</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">620</subfield><subfield code="q">ASE</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">620</subfield><subfield code="q">ASE</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Intra, Panich</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Evaluation of the Performance in Charging Efficiencies and Losses of Ultrafine Particles Ranging in Sizes from 15 to 75 nm in a Unipolar Corona-based Ionizer</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2020</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract For this study, a unipolar corona-based ionizer was constructed and experimentally evaluated for charging efficiencies and losses of ultrafine particles in the size range of 15–75 nm at different corona voltage, ion trap voltage and particle flow rate. The corona voltage was applied to the ionizer between 2.0–3.0 kV. The discharge currents increased from 0.16 nA to 4.23 μA and the ion number concentration increased from 6.27 × $ 10^{9} $ to 1.36 × $ 10^{14} $ ions/$ m^{3} $. Increasing the corona voltage lead to a higher discharge current and ion number concentration in the ionizer. The best intrinsic charging efficiency of the ionizer was about 92.15–99.33% for particle diameters ranging from 15 to 75 nm, and occurred at corona voltage, ion trap voltage and particle flow rate of about 3.0 kV, 100 V, 0.6 L/min, respectively. At a given corona voltage, the extrinsic charging efficiency increased as the particle flow rate increased. The best extrinsic charging efficiency ranged from 14.93 to 57.70% for particle diameters increasing from 15 to 75 nm, and occurred at corona voltage, ion trap voltage and particle flow rate of about 2.6 kV, 100 V, and 1.5 L/min, respectively. In the present ionizer, the highest electrostatic loss was observed for particles with a diameter of about 45 nm, and it was about 88.03% at a corona voltage of 3.0 kV and an ion trap voltage of 200 V. 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author |
Intra, Panich |
spellingShingle |
Intra, Panich ddc 620 misc Corona discharge misc Particle charging misc Particle ionizer misc Particle loss misc Charging efficiency Evaluation of the Performance in Charging Efficiencies and Losses of Ultrafine Particles Ranging in Sizes from 15 to 75 nm in a Unipolar Corona-based Ionizer |
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2093-7423 |
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620 ASE Evaluation of the Performance in Charging Efficiencies and Losses of Ultrafine Particles Ranging in Sizes from 15 to 75 nm in a Unipolar Corona-based Ionizer Corona discharge (dpeaa)DE-He213 Particle charging (dpeaa)DE-He213 Particle ionizer (dpeaa)DE-He213 Particle loss (dpeaa)DE-He213 Charging efficiency (dpeaa)DE-He213 |
topic |
ddc 620 misc Corona discharge misc Particle charging misc Particle ionizer misc Particle loss misc Charging efficiency |
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ddc 620 misc Corona discharge misc Particle charging misc Particle ionizer misc Particle loss misc Charging efficiency |
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ddc 620 misc Corona discharge misc Particle charging misc Particle ionizer misc Particle loss misc Charging efficiency |
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Evaluation of the Performance in Charging Efficiencies and Losses of Ultrafine Particles Ranging in Sizes from 15 to 75 nm in a Unipolar Corona-based Ionizer |
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(DE-627)SPR043373550 (DE-599)SPRs42835-020-00623-2-e (SPR)s42835-020-00623-2-e |
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Evaluation of the Performance in Charging Efficiencies and Losses of Ultrafine Particles Ranging in Sizes from 15 to 75 nm in a Unipolar Corona-based Ionizer |
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Intra, Panich |
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Intra, Panich Wanusbodeepaisarn, Paisarn Siri-achawawath, Thanesvorn |
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10.1007/s42835-020-00623-2 |
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verfasserin |
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evaluation of the performance in charging efficiencies and losses of ultrafine particles ranging in sizes from 15 to 75 nm in a unipolar corona-based ionizer |
title_auth |
Evaluation of the Performance in Charging Efficiencies and Losses of Ultrafine Particles Ranging in Sizes from 15 to 75 nm in a Unipolar Corona-based Ionizer |
abstract |
Abstract For this study, a unipolar corona-based ionizer was constructed and experimentally evaluated for charging efficiencies and losses of ultrafine particles in the size range of 15–75 nm at different corona voltage, ion trap voltage and particle flow rate. The corona voltage was applied to the ionizer between 2.0–3.0 kV. The discharge currents increased from 0.16 nA to 4.23 μA and the ion number concentration increased from 6.27 × $ 10^{9} $ to 1.36 × $ 10^{14} $ ions/$ m^{3} $. Increasing the corona voltage lead to a higher discharge current and ion number concentration in the ionizer. The best intrinsic charging efficiency of the ionizer was about 92.15–99.33% for particle diameters ranging from 15 to 75 nm, and occurred at corona voltage, ion trap voltage and particle flow rate of about 3.0 kV, 100 V, 0.6 L/min, respectively. At a given corona voltage, the extrinsic charging efficiency increased as the particle flow rate increased. The best extrinsic charging efficiency ranged from 14.93 to 57.70% for particle diameters increasing from 15 to 75 nm, and occurred at corona voltage, ion trap voltage and particle flow rate of about 2.6 kV, 100 V, and 1.5 L/min, respectively. In the present ionizer, the highest electrostatic loss was observed for particles with a diameter of about 45 nm, and it was about 88.03% at a corona voltage of 3.0 kV and an ion trap voltage of 200 V. Finally, the highest diffusion loss of about 22.66% was seen to occur with singly charged particles with a diameter of 15 nm at the particle flow rate of about 0.6 L/min. |
abstractGer |
Abstract For this study, a unipolar corona-based ionizer was constructed and experimentally evaluated for charging efficiencies and losses of ultrafine particles in the size range of 15–75 nm at different corona voltage, ion trap voltage and particle flow rate. The corona voltage was applied to the ionizer between 2.0–3.0 kV. The discharge currents increased from 0.16 nA to 4.23 μA and the ion number concentration increased from 6.27 × $ 10^{9} $ to 1.36 × $ 10^{14} $ ions/$ m^{3} $. Increasing the corona voltage lead to a higher discharge current and ion number concentration in the ionizer. The best intrinsic charging efficiency of the ionizer was about 92.15–99.33% for particle diameters ranging from 15 to 75 nm, and occurred at corona voltage, ion trap voltage and particle flow rate of about 3.0 kV, 100 V, 0.6 L/min, respectively. At a given corona voltage, the extrinsic charging efficiency increased as the particle flow rate increased. The best extrinsic charging efficiency ranged from 14.93 to 57.70% for particle diameters increasing from 15 to 75 nm, and occurred at corona voltage, ion trap voltage and particle flow rate of about 2.6 kV, 100 V, and 1.5 L/min, respectively. In the present ionizer, the highest electrostatic loss was observed for particles with a diameter of about 45 nm, and it was about 88.03% at a corona voltage of 3.0 kV and an ion trap voltage of 200 V. Finally, the highest diffusion loss of about 22.66% was seen to occur with singly charged particles with a diameter of 15 nm at the particle flow rate of about 0.6 L/min. |
abstract_unstemmed |
Abstract For this study, a unipolar corona-based ionizer was constructed and experimentally evaluated for charging efficiencies and losses of ultrafine particles in the size range of 15–75 nm at different corona voltage, ion trap voltage and particle flow rate. The corona voltage was applied to the ionizer between 2.0–3.0 kV. The discharge currents increased from 0.16 nA to 4.23 μA and the ion number concentration increased from 6.27 × $ 10^{9} $ to 1.36 × $ 10^{14} $ ions/$ m^{3} $. Increasing the corona voltage lead to a higher discharge current and ion number concentration in the ionizer. The best intrinsic charging efficiency of the ionizer was about 92.15–99.33% for particle diameters ranging from 15 to 75 nm, and occurred at corona voltage, ion trap voltage and particle flow rate of about 3.0 kV, 100 V, 0.6 L/min, respectively. At a given corona voltage, the extrinsic charging efficiency increased as the particle flow rate increased. The best extrinsic charging efficiency ranged from 14.93 to 57.70% for particle diameters increasing from 15 to 75 nm, and occurred at corona voltage, ion trap voltage and particle flow rate of about 2.6 kV, 100 V, and 1.5 L/min, respectively. In the present ionizer, the highest electrostatic loss was observed for particles with a diameter of about 45 nm, and it was about 88.03% at a corona voltage of 3.0 kV and an ion trap voltage of 200 V. Finally, the highest diffusion loss of about 22.66% was seen to occur with singly charged particles with a diameter of 15 nm at the particle flow rate of about 0.6 L/min. |
collection_details |
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container_issue |
2 |
title_short |
Evaluation of the Performance in Charging Efficiencies and Losses of Ultrafine Particles Ranging in Sizes from 15 to 75 nm in a Unipolar Corona-based Ionizer |
url |
https://dx.doi.org/10.1007/s42835-020-00623-2 |
remote_bool |
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author2 |
Wanusbodeepaisarn, Paisarn Siri-achawawath, Thanesvorn |
author2Str |
Wanusbodeepaisarn, Paisarn Siri-achawawath, Thanesvorn |
ppnlink |
519202015 |
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hochschulschrift_bool |
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doi_str |
10.1007/s42835-020-00623-2 |
up_date |
2024-07-03T18:15:05.062Z |
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|
score |
7.399081 |