{"data":{"id":"10.4121/71017f12-a3de-4cab-89a8-164384696004","type":"dois","attributes":{"doi":"10.4121/71017f12-a3de-4cab-89a8-164384696004","prefix":"10.4121","suffix":"71017f12-a3de-4cab-89a8-164384696004","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Gillmeier, Stefanie","givenName":"Stefanie","familyName":"Gillmeier","affiliation":[],"nameIdentifiers":[]},{"name":"Radhakrishnan Jayakumari, Anjali","nameType":"Personal","givenName":"Anjali","familyName":"Radhakrishnan Jayakumari","nameIdentifiers":[{"nameIdentifier":"0000-0002-4064-2820","nameIdentifierScheme":"https://orcid.org/"}],"affiliation":[]}],"titles":[{"title":"ERIES-Pollution, Atmospheric Boundary layer, Interaction and Ship Emission Data"}],"publisher":"4TU.ResearchData","container":{},"publicationYear":2025,"subjects":[{"subject":"Water Transport","subjectScheme":"Australian and New Zealand Standard Research Classification (ANZSRC), 2008","classificationCode":"8802"},{"subject":"Air Quality","subjectScheme":"Australian and New Zealand Standard Research Classification (ANZSRC), 2008","classificationCode":"9601"},{"subject":"Transport","subjectScheme":"Australian and New Zealand Standard Research Classification (ANZSRC), 2008","classificationCode":"88"},{"subject":"Environment","subjectScheme":"Australian and New Zealand Standard Research Classification (ANZSRC), 2008","classificationCode":"96"},{"subject":"Pollutant Dispersion"},{"subject":"Ship Emissions"},{"subject":"Buoyant Release"},{"subject":"Ship-Ship Interaction'"},{"subject":"Ship-Harbour Interaction"},{"subject":"Isolated Ship"}],"contributors":[{"name":"TU Eindhoven, Department Of The Built Environment, Building Physics And Services","nameType":"Organizational","affiliation":[],"contributorType":"Other","nameIdentifiers":[]},{"name":"Damen Naval","nameType":"Organizational","affiliation":[],"contributorType":"Other","nameIdentifiers":[]},{"name":"BlueOASIS-Ocean Sustainable Solutions","nameType":"Organizational","affiliation":[],"contributorType":"Other","nameIdentifiers":[]},{"name":"Knud E. Hansen","nameType":"Organizational","affiliation":[],"contributorType":"Other","nameIdentifiers":[]}],"dates":[{"date":"2025-06-10","dateType":"Issued"}],"language":"en","types":{"ris":"DATA","bibtex":"misc","citeproc":"dataset","schemaOrg":"Dataset","resourceType":"Dataset","resourceTypeGeneral":"Dataset"},"relatedIdentifiers":[{"relationType":"IsVersionOf","relatedIdentifier":"10.4121/71017f12-a3de-4cab-89a8-164384696004.v1","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":[],"formats":["'pdf' 'stp' 'png' 'jpg' 'xlsx' 'm (Matlab)' 'asA' 'thA' 'tdms' 'txt'"],"version":"1","rightsList":[{"rights":"Creative Commons Attribution 4.0 International","rightsUri":"https://creativecommons.org/licenses/by/4.0/legalcode","schemeUri":"https://spdx.org/licenses/","rightsIdentifier":"cc-by-4.0","rightsIdentifierScheme":"SPDX"}],"descriptions":[{"description":"The dispersion of pollutants exhausted from a generic service offshore vessel are investigated in the closed-circuit atmospheric boundary layer wind tunnel (ABLWT) at Eindhoven University of Technology. The vessel is replicated at a geometric scaling ratio of 1:100 and exposed to maritime neutral atmospheric flow conditions. For most measurements, an approach flow velocity of 10 m/s (full-scale) is set at the exhaust height.The majority of conducted measurements relate to 25% of maximum continuous rating (MCR) engine load, which results in a release velocity of Ue = 8.8 m/s (full-scale). Emissions are released from an exhaust with circular shaft of 0.76 m in diameter (De). To match the densimetric Froude number (Fr) in experiments, and reality, a velocity scaling ratio of 1:10 is chosen for the wind tunnel measurements.Main focus of pollutant concentration measurements is set on locations at 1.5 m height on the vessel’s deck to assess the possibility of workers’ exposure to emitted pollutants.Measurements are valid for the following conditions:• Standard atmospheric conditions (15 degrees Celsius and 1013.25 hPa), resulting in an ambient air density of ρa = 1.225 kg/m3.• Emission temperature of 350 degrees Celsius (corresponding to an emission density of 0.567 kg/m3)This results in a densymetric Froude number of Fr = 4.396069 (based on the diameter of the exhaust stack (De) and Ue = 8.8 m/s.\u003cbr\u003eIn addition to the Metadata report, raw data time series of pollutant concentrations as well as appraoch flow conditions are provided here.","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[{"awardTitle":"ERIES - Engineering Research Infrastructures for European Synergies","funderName":"European Union’s Horizon Europe Framework Programme","awardNumber":"Grant Agreement No. 101058684."}],"xml":"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