Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/108093
DC FieldValueLanguage
dc.contributorDepartment of Building Environment and Energy Engineering-
dc.creatorXing, Cen_US
dc.creatorAi, Zen_US
dc.creatorLiu, Zen_US
dc.creatorMak, CMen_US
dc.creatorWong, HMen_US
dc.date.accessioned2024-07-24T02:26:54Z-
dc.date.available2024-07-24T02:26:54Z-
dc.identifier.issn0360-1323en_US
dc.identifier.urihttp://hdl.handle.net/10397/108093-
dc.language.isoenen_US
dc.publisherElsevier BVen_US
dc.subjectDropletsen_US
dc.subjectLaser light scatteringen_US
dc.subjectParticle image velocimetryen_US
dc.subjectPowder-jet-handpiecesen_US
dc.subjectUltrasonic scaling instrumenten_US
dc.titleCharacteristics of droplets emission immediately around mouth during dental treatmentsen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.volume248en_US
dc.identifier.doi10.1016/j.buildenv.2023.111066en_US
dcterms.abstractControl measures aiming for removing droplets generated during dental treatments have been attracted increasing attention after COVID-19 pandemic, but the emission characteristics of droplets around the source (namely, the mouth) have still not been fully understood. The present study investigated experimentally the emission characteristics of droplets around mouth during typical dental treatments. A manikin being treated by portable dental instruments simulated the dental treatments, while the laser light scattering technique and particle image velocimetry (PIV) technique were employed to perform the measurements. The peak mass fraction of droplets occurs around the droplet size from 20 μ diameter less than 200 droplets ( μ m to 100 μ m, while the mass fraction of droplets with the m accounts for over 80 %. By fitting with the Rosin-Rammler equation, the mean size of ◦ to 83 ◦ d) are 54.96 and 98.93, and the size distribution parameter (n) are 1.35 and 1.58, respectively, for the process of air-powder-polishing and ultrasonic scaling. The dominant emission direction of droplets is towards the dummy’ head and chest. The emitted droplets formed approximately a cone shape, and its angle varied from 25 for different conditions. The maximum velocity of droplets at the location near the dummy’s mouth exceeds 1.0 m/s for most conditions. The injecting flow rate and treated tooth position are the major factors influencing the emission direction, angle, and velocity. It is expected that the results can further increase our understanding of emission characteristics of droplets and provide accurate initial conditions for CFD simulations.-
dcterms.accessRightsembargoed accessen_US
dcterms.bibliographicCitationBuilding and environment, 15 Jan. 2024, v. 248, 111066en_US
dcterms.isPartOfBuilding and environmenten_US
dcterms.issued2024-01-15-
dc.identifier.scopus2-s2.0-85178665702-
dc.identifier.eissn1873-684Xen_US
dc.identifier.artn111066en_US
dc.description.validate202407 bcch-
dc.identifier.FolderNumbera3079-
dc.identifier.SubFormID49400-
dc.description.fundingSourceOthersen_US
dc.description.fundingTextFundamental Research Funds for the Central Universities (No. 531118010378)en_US
dc.description.pubStatusPublisheden_US
dc.date.embargo2026-01-15en_US
dc.description.oaCategoryGreen (AAM)en_US
Appears in Collections:Journal/Magazine Article
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Embargo End Date 2026-01-15
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