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dc.contributor.authorLai, Kwan Tsaan
dc.contributor.authorWaite, Michael L
dc.date.accessioned2021-10-19 19:52:40 (GMT)
dc.date.available2021-10-19 19:52:40 (GMT)
dc.date.issued2020-07-08
dc.identifier.urihttps://doi.org/10.1175/MWR-D-19-0330.1
dc.identifier.urihttp://hdl.handle.net/10012/17655
dc.description© Copyright 2020 American Meteorological Society (AMS). For permission to reuse any portion of this work, please contact permissions@ametsoc.org. Any use of material in this work that is determined to be “fair use” under Section 107 of the U.S. Copyright Act (17 U.S. Code §?107) or that satisfies the conditions specified in Section 108 of the U.S. Copyright Act (17 USC § 108) does not require the AMS’s permission. Republication, systematic reproduction, posting in electronic form, such as on a website or in a searchable database, or other uses of this material, except as exempted by the above statement, requires written permission or a license from the AMS. All AMS journals and monograph publications are registered with the Copyright Clearance Center (https://www.copyright.com). Additional details are provided in the AMS Copyright Policy statement, available on the AMS website (https://www.ametsoc.org/PUBSCopyrightPolicy).en
dc.description.abstractIn this paper, the sensitivity of idealized squall-line simulations to horizontal resolution, subgrid turbulence mixing scheme, and subfilter-scale motion is discussed. Inconsistent results from numerical simulations of convective systems have suggested that there are issues with the behavior of the subgrid turbulent mixing parameterizations with increasing resolution that still need to be understood. WRF is used to perform large eddy simulation of an idealized squall line with horizontal grid spacings of 4 km, 2 km, 1 km, 500 m, and 250 m. While 4 km grid spacing is able to produce the general structure of the squall line, higher-resolution simu lations produce more detailed structures. Individual convective cell size decreases, the maximum cloud top height increases, and the subgrid turbulence kinetic energy (TKE) ratio decreases as resolution increases. As found in past studies, 4 km grid spacing is not recommended as it contains an unreasonable amount of subgrid TKE, is not sufficient to resolve the large energy-containing eddies, and may even suppress propagation of the squall line. While horizontal resolution of 1 km can produce a squall line, there are several discrepancies between the 1 km case and higher resolutions, including trailing banded structures and inhibited three dimensionalization. These issues at 1 km resolution are investigated by examining the subfilter energy transfer for the highest-resolution simulation filtered to a horizontal scale of 1 km. The subfilter energy transfer rate at a scale of 1 km is dominated by the streamwise and shear components. While dissipation dominates the transfer, a significant amount of backscatter also exists, which is not represented by most subgrid models.en
dc.description.sponsorshipFunder 1, Natural Sciences and Engineering Research Council of Canada (Grant RGPIN-386456-2015) || Funder 2, and the Canadian Foundation for Innovation.en
dc.language.isoenen
dc.publisherAMSen
dc.relation.ispartofseriesMonthly Weather Review;
dc.subjectCloud resolving modelsen
dc.subjectParameterizationen
dc.subjectSubgrid-scale processesen
dc.titleResolution Dependence and Subfilter-Scale Motions in Idealized Squall-Line Simulationsen
dc.typeArticleen
dcterms.bibliographicCitationLai, K. T., & Waite, M. L. (2020). Resolution Dependence and Subfilter-Scale Motions in Idealized Squall-Line Simulations. Monthly Weather Review, 148(7), 3059–3078. https://doi.org/10.1175/MWR-D-19-0330.1en
uws.contributor.affiliation1Faculty of Mathematicsen
uws.contributor.affiliation2Applied Mathematicsen
uws.typeOfResourceTexten
uws.peerReviewStatusRevieweden
uws.scholarLevelFacultyen


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