Mechanisms and time scales of glacial inception simulated with an Earth system model of intermediate complexity

dc.bibliographicCitation.firstPage245eng
dc.bibliographicCitation.issue2eng
dc.bibliographicCitation.lastPage258eng
dc.bibliographicCitation.volume5
dc.contributor.authorCalov, R.
dc.contributor.authorGanopolski, A.
dc.contributor.authorKubatzki, C.
dc.contributor.authorClaussen, M.
dc.date.accessioned2018-08-28T00:06:48Z
dc.date.available2019-06-26T17:18:54Z
dc.date.issued2009
dc.description.abstractWe investigate glacial inception and glacial thresholds in the climate-cryosphere system utilising the Earth system model of intermediate complexity CLIMBER-2, which includes modules for atmosphere, terrestrial vegetation, ocean and interactive ice sheets. The latter are described by the three-dimensional polythermal ice-sheet model SICOPOLIS. A bifurcation which represents glacial inception is analysed with two different model setups: one setup with dynamical ice-sheet model and another setup without it. The respective glacial thresholds differ in terms of maximum boreal summer insolation at 65° N (hereafter referred as Milankovitch forcing (MF)). The glacial threshold of the configuration without ice-sheet dynamics corresponds to a much lower value of MF compared to the full model. If MF attains values only slightly below the aforementioned threshold there is fast transient response. Depending on the value of MF relative to the glacial threshold, the transient response time of inland-ice volume in the model configuration with ice-sheet dynamics ranges from 10 000 to 100 000 years. Due to these long response times, a glacial threshold obtained in an equilibrium simulation is not directly applicable to the transient response of the climate-cryosphere system to time-dependent orbital forcing. It is demonstrated that in transient simulations just crossing of the glacial threshold does not imply large-scale glaciation of the Northern Hemisphere. We found that in transient simulations MF has to drop well below the glacial threshold determined in an equilibrium simulation to initiate glacial inception. Finally, we show that the asynchronous coupling between climate and inland-ice components allows one sufficient realistic simulation of glacial inception and, at the same time, a considerable reduction of computational costs.eng
dc.description.versionpublishedVersioneng
dc.formatapplication/pdf
dc.identifier.urihttps://doi.org/10.34657/1103
dc.identifier.urihttps://oa.tib.eu/renate/handle/123456789/625
dc.language.isoengeng
dc.publisherMünchen : European Geopyhsical Unioneng
dc.relation.doihttps://doi.org/10.5194/cp-5-245-2009
dc.relation.ispartofseriesClimate of the Past, Volume 5, Issue 2, Page 245-258eng
dc.rights.licenseCC BY 3.0 Unportedeng
dc.rights.urihttps://creativecommons.org/licenses/by/3.0/eng
dc.subjectcryosphereeng
dc.subjectglacier dynamicseng
dc.subjectglaciologyeng
dc.subjectice sheeteng
dc.subjectNorthern Hemisphereeng
dc.subjectnumerical modeleng
dc.subjectorbital forcingeng
dc.subject.ddc550eng
dc.titleMechanisms and time scales of glacial inception simulated with an Earth system model of intermediate complexityeng
dc.typearticleeng
dc.typeTexteng
dcterms.bibliographicCitation.journalTitleClimate of the Pasteng
tib.accessRightsopenAccesseng
wgl.contributorPIKeng
wgl.subjectGeowissenschafteneng
wgl.typeZeitschriftenartikeleng
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