Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/112009
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dc.contributorDepartment of Civil and Environmental Engineeringen_US
dc.creatorWang, Cen_US
dc.creatorXu, Jen_US
dc.creatorZhai, Hen_US
dc.creatorSo, LKen_US
dc.creatorGuo, Hen_US
dc.date.accessioned2025-03-21T02:22:48Z-
dc.date.available2025-03-21T02:22:48Z-
dc.identifier.issn0304-3894en_US
dc.identifier.urihttp://hdl.handle.net/10397/112009-
dc.language.isoenen_US
dc.publisherElsevieren_US
dc.rights© 2025 The Author(s). Published by Elsevier B.V. This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/4.0/).en_US
dc.rightsThe following publication Wang, C., Xu, J., Zhai, H., So, L. K., & Guo, H. (2025). Mapping full-range infection transmission from speaking, coughing, and sneezing in indoor environments and its impact on social distancing. Journal of Hazardous Materials, 490, 137782 is available at https://dx.doi.org/10.1016/j.jhazmat.2025.137782.en_US
dc.subjectCOVID −19en_US
dc.subjectDose-response modelen_US
dc.subjectDroplet dispersionen_US
dc.subjectInfection risken_US
dc.subjectPenetration distanceen_US
dc.titleMapping full-range infection transmission from speaking, coughing, and sneezing in indoor environments and its impact on social distancingen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.volume490en_US
dc.identifier.doi10.1016/j.jhazmat.2025.137782en_US
dcterms.abstractInfectious respiratory diseases have posed significant threats to public health in the past decades. However, the full-range transmission in indoor environments remains unclear. In this study, we used the computational fluid dynamics (CFD) method with the large eddy simulation (LES) model, validated by particle image velocimetry (PIV) experiments, to explore the full-range transmission in an indoor space. The penetration of airborne droplets was divided into five power-law phases: accelerating jet (< 0.04–0.1 s, 0.3 m), decelerating jet (< 0.2–0.6 s, 0.7 m), puff (< 20 s, 2.2–3.8 m), mixing (< 360 s), and well-mixed phases (> 360 s). The maximum travel distance versus droplet diameter indicated “V” shapes, with minimum distances of 0.5–1.3 m for 100 µm droplets. The virus concentration decreased exponentially with distance and sustained high values within 2.8 m as a cone shape. The safe distance with an infection risk threshold of 10 % varied from 1 to 4 m, depending on viral load, dwell time, and mask. Here, we suggest social distances of 1, 1.8, and 4 m for the mask and asymptomatic cases, a short duration of viral loads < 107 #/mL, and a short duration of viral loads of 108–9 #/mL or long duration, respectively.en_US
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationJournal of hazardous materials, 15 June 2025, v. 490, 137782en_US
dcterms.isPartOfJournal of hazardous materialsen_US
dcterms.issued2025-06-15-
dc.identifier.scopus2-s2.0-85218885566-
dc.identifier.eissn1873-3336en_US
dc.identifier.artn137782en_US
dc.description.validate202503 bcwcen_US
dc.description.oaVersion of Recorden_US
dc.identifier.FolderNumberOA_TA-
dc.description.fundingSourceRGCen_US
dc.description.fundingSourceOthersen_US
dc.description.fundingTextHong Kong Polytechnic Universityen_US
dc.description.pubStatusPublisheden_US
dc.description.TAElsevier (2025)en_US
dc.description.oaCategoryTAen_US
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