Analyzing the atmospheric boundary layer using high-order moments obtained from multiwavelength lidar data

dc.contributor.authorMOREIRA, GREGORI de A.pt_BR
dc.contributor.authorLOPES, FABIO J. da S.pt_BR
dc.contributor.authorGUERRERO-RASCADO, JUAN L.pt_BR
dc.contributor.authorSILVA, JONATAN J. dapt_BR
dc.contributor.authorGOMES, ANTONIO A.pt_BR
dc.contributor.authorLANDULFO, EDUARDOpt_BR
dc.contributor.authorALADOS-ARBOLEDAS, LUCASpt_BR
dc.coverageInternacionalpt_BR
dc.date.accessioned2019-11-29T11:19:15Z
dc.date.available2019-11-29T11:19:15Z
dc.date.issued2019pt_BR
dc.description.abstractThe lowest region of the troposphere is a turbulent layer known as the atmospheric boundary layer (ABL) and characterized by high daily variability due to the influence of surface forcings. This is the reason why detecting systems with high spatial and temporal resolution, such as lidar, have been widely applied for researching this region. In this paper, we present a comparative analysis on the use of lidar-backscattered signals at three wavelengths (355, 532 and 1064 nm) to study the ABL by investigating the highorder moments, which give us information about the ABL height (derived by the variance method), aerosol layer movement (skewness) and mixing conditions (kurtosis) at several heights. Previous studies have shown that the 1064 nm wavelength, due to the predominance of particle signature in the total backscattered atmospheric signal and practically null presence of molecular signal (which can represent noise in high-order moments), provides an appropriate description of the turbulence field, and thus in this study it was considered a reference. We analyze two case studies that show us that the backscattered signal at 355 nm, even after applying some corrections, has a limited applicability for turbulence studies using the proposed methodology due to the strong contribution of the molecular signature to the total backscatter signal. This increases the noise associated with the high-order profiles and, consequently, generates misinformation. On the other hand, the information on the turbulence field derived from the backscattered signal at 532 nm is similar to that obtained at 1064 nm due to the appropriate attenuation of the noise, generated by molecular component of backscattered signal by the application of the corrections proposed.pt_BR
dc.description.sponsorshipConselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)pt_BR
dc.description.sponsorshipFundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)pt_BR
dc.description.sponsorshipIDCNPq: 152156/2018-6; 432515/2018-6; 150716/2017-6pt_BR
dc.description.sponsorshipIDFAPESP: 15/12793-0pt_BR
dc.format.extent4261-4276pt_BR
dc.identifier.citationMOREIRA, GREGORI de A.; LOPES, FABIO J. da S.; GUERRERO-RASCADO, JUAN L.; SILVA, JONATAN J. da; GOMES, ANTONIO A.; LANDULFO, EDUARDO; ALADOS-ARBOLEDAS, LUCAS. Analyzing the atmospheric boundary layer using high-order moments obtained from multiwavelength lidar data: impact of wavelength choice. <b>Atmospheric Measurement Techniques</b>, v. 12, n. 8, p. 4261-4276, 2019. DOI: <a href="https://dx.doi.org/10.5194/amt-12-4261-2019">10.5194/amt-12-4261-2019</a>. Disponível em: http://repositorio.ipen.br/handle/123456789/30379.
dc.identifier.doi10.5194/amt-12-4261-2019pt_BR
dc.identifier.fasciculo8pt_BR
dc.identifier.issn1867-1381pt_BR
dc.identifier.orcid0000-0002-9691-5306pt_BR
dc.identifier.orcidhttps://orcid.org/0000-0002-9691-5306
dc.identifier.percentilfi71.505pt_BR
dc.identifier.percentilfiCiteScore82.00
dc.identifier.urihttp://repositorio.ipen.br/handle/123456789/30379
dc.identifier.vol12pt_BR
dc.relation.ispartofAtmospheric Measurement Techniquespt_BR
dc.rightsopenAccesspt_BR
dc.subjecttroposphere
dc.subjectoptical radar
dc.subjectboundary layers
dc.subjectatmospheres
dc.subjectaerosols
dc.subjectturbulence
dc.subjectair quality
dc.subjectmonitoring
dc.titleAnalyzing the atmospheric boundary layer using high-order moments obtained from multiwavelength lidar datapt_BR
dc.typeArtigo de periódicopt_BR
dspace.entity.typePublication
ipen.autorJONATAN JOÃO DA SILVA
ipen.autorANTONIO ARLEQUES GOMES
ipen.autorEDUARDO LANDULFO
ipen.autorFABIO JULIANO DA SILVA LOPES
ipen.autorGREGORI DE ARRUDA MOREIRA
ipen.codigoautor14389
ipen.codigoautor14258
ipen.codigoautor503
ipen.codigoautor6576
ipen.codigoautor10204
ipen.contributor.ipenauthorJONATAN JOÃO DA SILVA
ipen.contributor.ipenauthorANTONIO ARLEQUES GOMES
ipen.contributor.ipenauthorEDUARDO LANDULFO
ipen.contributor.ipenauthorFABIO JULIANO DA SILVA LOPES
ipen.contributor.ipenauthorGREGORI DE ARRUDA MOREIRA
ipen.date.recebimento19-11
ipen.identifier.fi3.668pt_BR
ipen.identifier.fiCiteScore6.3
ipen.identifier.ipendoc26404pt_BR
ipen.identifier.iwosWoSpt_BR
ipen.range.fi3.000 - 4.499
ipen.range.percentilfi50.00 - 74.99
ipen.subtituloimpact of wavelength choicept_BR
ipen.type.genreArtigo
relation.isAuthorOfPublication6220a82d-6d12-4333-9853-7a36f1814bf5
relation.isAuthorOfPublicationca91cf97-565f-47d6-adb8-cd9d2cdadc9b
relation.isAuthorOfPublicatione4dff370-e8c1-4437-846a-ef18a3ad606b
relation.isAuthorOfPublicationdbeb371a-361e-499e-a0ab-4826638fb1ca
relation.isAuthorOfPublication539c9881-45aa-4cc9-aefe-a503026f1567
relation.isAuthorOfPublication.latestForDiscovery539c9881-45aa-4cc9-aefe-a503026f1567
sigepi.autor.atividadeLANDULFO, EDUARDO:503:920:Npt_BR
sigepi.autor.atividadeGOMES, ANTONIO A.:14258:920:Npt_BR
sigepi.autor.atividadeSILVA, JONATAN J. da:14389:920:Npt_BR
sigepi.autor.atividadeLOPES, FABIO J. da S.:6576:920:Npt_BR
sigepi.autor.atividadeMOREIRA, GREGORI de A.:10204:920:Spt_BR

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