Vis enkel innførsel

dc.contributor.authorDuarte, Pedro
dc.contributor.authorBrændshøi, Jostein
dc.contributor.authorShcherbin, Dmitry
dc.contributor.authorBarras, Pauline
dc.contributor.authorAlbretsen, Jon
dc.contributor.authorGusdal, Yvonne
dc.contributor.authorSzapiro, Nicholas
dc.contributor.authorMartinsen, Andreas Rostrup
dc.contributor.authorSamuelsen, Annette
dc.contributor.authorWang, Keguang
dc.contributor.authorDebernard, Jens Boldingh
dc.date.accessioned2022-09-20T08:15:10Z
dc.date.available2022-09-20T08:15:10Z
dc.date.created2022-06-09T08:22:39Z
dc.date.issued2022
dc.identifier.citationGeoscientific Model Development. 2022, 15 (11), 4373-4392.
dc.identifier.issn1991-959X
dc.identifier.urihttps://hdl.handle.net/11250/3019046
dc.description.abstractThe Los Alamos Sea Ice Model (CICE) is used by several Earth system models where sea ice boundary conditions are not necessary, given their global scope. However, regional and local implementations of sea ice models require boundary conditions describing the time changes of the sea ice and snow being exchanged across the boundaries of the model domain. The physical detail of these boundary conditions regarding, for example, the usage of different sea ice thickness categories or the vertical resolution of thermodynamic properties, must be considered when matching them with the requirements of the sea ice model. Available satellite products do not include all required data. Therefore, the most straightforward way of getting sea ice boundary conditions is from a larger-scale model. The main goal of our study is to describe and evaluate the implementation of time-varying sea ice boundaries in the CICE model using two regional coupled ocean–sea ice models, both covering a large part of the Barents Sea and areas around Svalbard: the Barents-2.5 km, implemented at the Norwegian Meteorological Institute (MET), and the Svalbard 4 km (S4K) model, implemented at the Norwegian Polar Institute (NPI). We use the TOPAZ4 model and a Pan-Arctic 4 km resolution model (A4) to generate the boundary conditions for the sea ice and the ocean. The Barents-2.5 km model is MET’s main forecasting model for ocean state and sea ice in the Barents Sea. The S4K model covers a similar domain but it is used mainly for research purposes. Obtained results show significant improvements in the performance of the Barents-2.5 km model after the implementation of the time-varying boundary conditions. The performance of the S4K model in terms of sea ice and snow thickness is comparable to that of the TOPAZ4 system but with more accurate results regarding the oceanic component because of using ocean boundary conditions from the A4 model. The implementation of time-varying boundary conditions described in this study is similar regardless of the CICE versions used in different models. The main challenge remains the handling of data from larger models before its usage as boundary conditions for regional/local sea ice models, since mismatches between available model products from the former and specific requirements of the latter are expected, implying case-specific approaches and different assumptions. Ideally, model setups should be as similar as possible to allow a smoother transition from larger to smaller domains.
dc.description.abstractImplementation and evaluation of open boundary conditions for sea ice in a regional coupled ocean (ROMS) and sea ice (CICE) modeling system
dc.language.isoeng
dc.subjectSjøis
dc.subjectSea ice
dc.subjectHavmodeller
dc.subjectOcean modelling
dc.subjectBiogeochemistry
dc.subjectBiogeochemistry
dc.titleImplementation and evaluation of open boundary conditions for sea ice in a regional coupled ocean (ROMS) and sea ice (CICE) modeling system
dc.title.alternativeImplementation and evaluation of open boundary conditions for sea ice in a regional coupled ocean (ROMS) and sea ice (CICE) modeling system
dc.typePeer reviewed
dc.typeJournal article
dc.description.versionpublishedVersion
dc.subject.nsiVDP::Andre geofag: 469
dc.subject.nsiVDP::Other geosciences: 469
dc.source.pagenumber4373-4392
dc.source.volume15
dc.source.journalGeoscientific Model Development
dc.source.issue11
dc.identifier.doi10.5194/gmd-15-4373-2022
dc.identifier.cristin2030353
dc.relation.projectSigma2: NN9300K
dc.relation.projectKlima- og miljødepartementet: 40241
dc.relation.projectEU – Horisont Europa (EC/HEU): 869154
dc.relation.projectEU – Horisont Europa (EC/HEU): 101003826
dc.relation.projectNorges forskningsråd: 276730
dc.relation.projectFramsenteret: 66200
cristin.ispublishedtrue
cristin.fulltextoriginal
cristin.qualitycode2


Tilhørende fil(er)

Thumbnail

Denne innførselen finnes i følgende samling(er)

Vis enkel innførsel