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dc.contributor.authorVergara-Temprado, J
dc.contributor.authorHolden, MA
dc.contributor.authorOrton, TR
dc.contributor.authorO'Sullivan, D
dc.contributor.authorUmo, NS
dc.contributor.authorBrowse, J
dc.contributor.authorReddington, C
dc.contributor.authorBaeza-Romero, MT
dc.contributor.authorJones, JM
dc.contributor.authorLea-Langton, A
dc.contributor.authorWilliams, A
dc.contributor.authorCarslaw, KS
dc.contributor.authorMurray, BJ
dc.date.accessioned2018-07-31T15:08:44Z
dc.date.issued2018-04-26
dc.description.abstractIt has been hypothesized that black carbon (BC) influences mixed-phase clouds by acting as an ice-nucleating particle (INP). However, the literature data for ice nucleation by BC immersed in supercooled water are extremely varied, with some studies reporting that BC is very effective at nucleating ice, whereas others report no ice-nucleating ability. Here we present new experimental results for immersion mode ice nucleation by BC from two contrasting fuels (n-decane and eugenol). We observe no significant heterogeneous nucleation by either sample. Using a global aerosol model, we quantify the maximum relative importance of BC for ice nucleation when compared with K-feldspar and marine organic aerosol acting as INP. Based on the upper limit from our laboratory data, we show that BC contributes at least several orders of magnitude less INP than feldspar and marine organic aerosol. Representations of its atmospheric ice-nucleating ability based on older laboratory data produce unrealistic results when compared against ambient observations of INP. Since BC is a complex material, it cannot be unambiguously ruled out as an important INP species in all locations at all times. Therefore, we use our model to estimate a range of values for the density of active sites that BC particles must have to be relevant for ice nucleation in the atmosphere. The estimated values will guide future work on BC, defining the required sensitivity of future experimental studies.en_GB
dc.description.sponsorshipThis study has been funded by the European Union’s Seventh Framework Programme (FP7/2007-797 2013) under grant agreement 603445 (BACCHUS), the European Research Council (ERC,240449 ICE and 648661 MarineIce), and the Engineering and Physical Sciences Research Council (EPSRC, EP/M003027/1). The global model simulations were performed on the ARCHER UK National Supercomputing Service. Ken S. Carslaw is a Royal Society Wolfson Merit Award holder. Nsikanabasi Umo acknowledges funding from the Niger Delta Development Commission (NDDC) in Nigeria (NDDC/DEHSS/ 2010PGFS/AK/011) and the Alexander von Humboldt Foundation, Germany (1188375).en_GB
dc.identifier.citationVol. 123, pp. 4273 - 4283en_GB
dc.identifier.doi10.1002/2017JD027831
dc.identifier.urihttp://hdl.handle.net/10871/33612
dc.language.isoenen_GB
dc.publisherAmerican Geophysical Union (AGU)en_GB
dc.relation.sourceAll the data used in this manuscript can be accessed at https://doi.org/10.5518/310en_GB
dc.relation.urlhttps://www.ncbi.nlm.nih.gov/pubmed/29938147en_GB
dc.rights© 2018 The Author(s). Open Access. This article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.en_GB
dc.subjectaerosolen_GB
dc.subjectblack carbonen_GB
dc.subjectcloudsen_GB
dc.subjectglobal modelingen_GB
dc.subjectice nucleationen_GB
dc.subjectmixed‐phase cloudsen_GB
dc.titleIs Black Carbon an Unimportant Ice-Nucleating Particle in Mixed-Phase Clouds?en_GB
dc.typeArticleen_GB
dc.date.available2018-07-31T15:08:44Z
dc.identifier.issn2169-897X
exeter.place-of-publicationUnited Statesen_GB
dc.descriptionThis is the final version of the article. Available from [publisher] via the DOI in this record.en_GB
dc.identifier.journalJournal of Geophysical Research: Atmospheresen_GB


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