Antarctic sub-shelf melt rates via PICO

dc.bibliographicCitation.firstPage1969eng
dc.bibliographicCitation.issue6eng
dc.bibliographicCitation.journalTitleThe Cryosphereeng
dc.bibliographicCitation.lastPage1985eng
dc.bibliographicCitation.volume12
dc.contributor.authorReese, Ronja
dc.contributor.authorAlbrecht, Torsten
dc.contributor.authorMengel, Matthias
dc.contributor.authorAsay-Davis, Xylar
dc.contributor.authorWinkelmann, Ricarda
dc.date.accessioned2018-09-01T12:07:08Z
dc.date.available2019-06-26T17:19:22Z
dc.date.issued2018
dc.description.abstractOcean-induced melting below ice shelves is one of the dominant drivers for mass loss from the Antarctic Ice Sheet at present. An appropriate representation of sub-shelf melt rates is therefore essential for model simulations of marine-based ice sheet evolution. Continental-scale ice sheet models often rely on simple melt-parameterizations, in particular for long-term simulations, when fully coupled ice–ocean interaction becomes computationally too expensive. Such parameterizations can account for the influence of the local depth of the ice-shelf draft or its slope on melting. However, they do not capture the effect of ocean circulation underneath the ice shelf. Here we present the Potsdam Ice-shelf Cavity mOdel (PICO), which simulates the vertical overturning circulation in ice-shelf cavities and thus enables the computation of sub-shelf melt rates consistent with this circulation. PICO is based on an ocean box model that coarsely resolves ice shelf cavities and uses a boundary layer melt formulation. We implement it as a module of the Parallel Ice Sheet Model (PISM) and evaluate its performance under present-day conditions of the Southern Ocean. We identify a set of parameters that yield two-dimensional melt rate fields that qualitatively reproduce the typical pattern of comparably high melting near the grounding line and lower melting or refreezing towards the calving front. PICO captures the wide range of melt rates observed for Antarctic ice shelves, with an average of about 0.1 m a−1 for cold sub-shelf cavities, for example, underneath Ross or Ronne ice shelves, to 16 m a−1 for warm cavities such as in the Amundsen Sea region. This makes PICO a computationally feasible and more physical alternative to melt parameterizations purely based on ice draft geometry.eng
dc.description.versionpublishedVersioneng
dc.formatapplication/pdf
dc.identifier.urihttps://doi.org/10.34657/804
dc.identifier.urihttps://oa.tib.eu/renate/handle/123456789/675
dc.language.isoengeng
dc.publisherMünchen : European Geopyhsical Unioneng
dc.relation.doihttps://doi.org/10.5194/tc-12-1969-2018
dc.rights.licenseCC BY 3.0 Unportedeng
dc.rights.urihttps://creativecommons.org/licenses/by/3.0/eng
dc.subject.ddc550eng
dc.subject.otherboundary layereng
dc.subject.othergrounding lineeng
dc.subject.otherice sheeteng
dc.subject.otherice shelfeng
dc.subject.otherice-ocean interactioneng
dc.subject.othericeberg calvingeng
dc.subject.otheroceanic circulationeng
dc.subject.othertwo-dimensional modelingeng
dc.titleAntarctic sub-shelf melt rates via PICOeng
dc.typeArticleeng
dc.typeTexteng
tib.accessRightsopenAccesseng
wgl.contributorPIKeng
wgl.subjectGeowissenschafteneng
wgl.typeZeitschriftenartikeleng
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