Simulation of Arctic sea ice within the DeepMIP Eocene ensemble: Thresholds, seasonality and factors controlling sea ice development

Igor Niezgodzki, Gregor Knorr, Gerrit Lohmann, Daniel J. Lunt, Christopher J. Poulsen, Sebastian Steinig, Jiang Zhu, Agatha De Boer, Wing-le Chan, Yannick Donnadieu, David K. Hutchinson, Jean-baptiste Ladant, Polina Morozova

Research output: Contribution to journalArticle (Academic Journal)peer-review

3 Citations (Scopus)

Abstract

The early Eocene greenhouse climate maintained by high atmospheric CO2 concentrations serves as a testbed for future climate changes dominated by increasing CO2 forcing. In particular, the early Eocene Arctic region is important in the context of future CO2 driven climate warming in the northern polar region and associated shrinking Arctic sea ice. Here, we present early Eocene Arctic sea ice simulations carried out by six coupled climate models within the framework of the Deep-Time Model Intercomparison Project (DeepMIP). We find differences in sea ice responses to CO2 changes across the ensemble and compare the results with available proxy-based sea ice reconstructions from the Arctic Ocean. Most of the models simulate seasonal sea ice presence at high CO2 levels (≥ 840 ppmv = 3× pre-industrial (PI) level of 280 ppmv). However, the threshold when sea ice permanently disappears from the ocean varies considerably between the models (from 1680 ppmv). Based on a one-dimensional energy balance model analysis we find that the greenhouse effect likely caused by increased atmospheric water vapor concentration plays an important role in the inter-model spread in Arctic winter surface temperature changes in response to a CO2 rise from 1× to 3× the PI level. Furthermore, differences in simulated surface salinity in the Arctic Ocean play an important role in the control of local sea ice formation. These differences result from different implementations of river run-off between the models, but also from differences in the exchange of waters between a brackish Arctic and a more saline North Atlantic Ocean that are controlled by the width of the gateway between both basins. As there is no geological evidence for Arctic sea ice in the early Eocene, its presence in most of the simulations with 3× PI CO2 level indicates either a higher CO2 level and/or an overly weak polar sensitivity in these models.
Original languageEnglish
Article number103848
JournalGlobal and Planetary Change
Volume214
DOIs
Publication statusPublished - 25 May 2022

Bibliographical note

Funding Information:
Igor Niezgodzki would like to thank Stefan Hagemann for the preparation of the. adjustments of the HD model for COSMOS Eocene setup. Igor Niezgodzki is grateful to the AWI Computing Center for providing the supercomputing resources for carrying out the simulations. Christopher J. Poulsen acknowledges funding through Heising Simon Foundation Award #2016-05 and NSF Award 2002397. Dan Lunt and Seb Steinig acknowledge the NERC SWEET grant, NE/P01903X/1. Agatha de Boer and David Hutchinson acknowledge support from Swedish Research Council projects 2016-03912 and 2020-04791, and FORMAS grant 2018-01621. Polina Morozova acknowledges support from the project FMGE-2019-0009 and thanks Evgeny Volodin and INM RAS for the help with INMCM simulations. GFDL numerical simulations were performed by resources provided by the Swedish National Infrastructure for Computing (SNIC) at the National Supercomputer Centre (NSC), partially funded by the Swedish Research Council through grant agreement no. 2018-05973. The CESM project is supported primarily by the National Science Foundation (NSF). This material is based upon work supported by the National Center for Atmospheric Research (NCAR), which is a major facility sponsored by the NSF under Cooperative Agreement No. 1852977.

Funding Information:
adjustments of the HD model for COSMOS Eocene setup. Igor Niezgodzki is grateful to the AWI Computing Center for providing the supercomputing resources for carrying out the simulations. Christopher J. Poulsen acknowledges funding through Heising Simon Foundation Award # 2016-05 and NSF Award 2002397 . Dan Lunt and Seb Steinig acknowledge the NERC SWEET grant, NE/P01903X/1 . Agatha de Boer and David Hutchinson acknowledge support from Swedish Research Council projects 2016-03912 and 2020-04791 , and FORMAS grant 2018-01621 . Polina Morozova acknowledges support from the project FMGE-2019-0009 and thanks Evgeny Volodin and INM RAS for the help with INMCM simulations. GFDL numerical simulations were performed by resources provided by the Swedish National Infrastructure for Computing (SNIC) at the National Supercomputer Centre (NSC), partially funded by the Swedish Research Council through grant agreement no. 2018-05973. The CESM project is supported primarily by the National Science Foundation (NSF). This material is based upon work supported by the National Center for Atmospheric Research (NCAR), which is a major facility sponsored by the NSF under Cooperative Agreement No. 1852977 .

Publisher Copyright:
© 2022

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  • SWEET NERC Large Grant

    Lunt, D. (Principal Investigator)

    1/10/1730/09/23

    Project: Research

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