Projecting Antarctica's contribution to future sea level rise from basal ice shelf melt using linear response functions of 16 ice sheet models (LARMIP-2)

Journal Article · Fri Feb 14 00:00:00 EST 2020 · Earth System Dynamics (Online)

DOI:https://doi.org/10.5194/esd-11-35-2020· OSTI ID:1599529

Levermann, Anders ; Winkelmann, Ricarda ; Albrecht, Torsten ; Goelzer, Heiko; Golledge, Nicholas R. ; Greve, Ralf ; Huybrechts, Philippe ; Jordan, Jim ; Leguy, Gunter; Martin, Daniel ; Morlighem, Mathieu ; Pattyn, Frank ; Pollard, David; Quiquet, Aurelien ; Rodehacke, Christian ; Seroussi, Helene ; Sutter, Johannes ; Zhang, Tong; Van Breedam, Jonas ; Calov, Reinhard ; DeConto, Robert; Dumas, Christophe; Garbe, Julius ; Gudmundsson, G. Hilmar ; Hoffman, Matthew J. ; Humbert, Angelika ; Kleiner, Thomas ; Lipscomb, William H.; Meinshausen, Malte ; Ng, Esmond; Nowicki, Sophie M. J.; Perego, Mauro; Price, Stephen F. ; Saito, Fuyuki ; Schlegel, Nicole-Jeanne ; Sun, Sainan; van de Wal, Roderik S. W.

The sea level contribution of the Antarctic ice sheet constitutes a large uncertainty in future sea level projections. Here we apply a linear response theory approach to 16 state-of-the-art ice sheet models to estimate the Antarctic ice sheet contribution from basal ice shelf melting within the 21st century. The purpose of this computation is to estimate the uncertainty of Antarctica's future contribution to global sea level rise that arises from large uncertainty in the oceanic forcing and the associated ice shelf melting. Ice shelf melting is considered to be a major if not the largest perturbation of the ice sheet's flow into the ocean. However, by computing only the sea level contribution in response to ice shelf melting, our study is neglecting a number of processes such as surface-mass-balance-related contributions. In assuming linear response theory, we are able to capture complex temporal responses of the ice sheets, but we neglect any self-dampening or self-amplifying processes. This is particularly relevant in situations in which an instability is dominating the ice loss. The results obtained here are thus relevant, in particular wherever the ice loss is dominated by the forcing as opposed to an internal instability, for example in strong ocean warming scenarios. In order to allow for comparison the methodology was chosen to be exactly the same as in an earlier study (Levermann et al., 2014) but with 16 instead of 5 ice sheet models. We include uncertainty in the atmospheric warming response to carbon emissions (full range of CMIP5 climate model sensitivities), uncertainty in the oceanic transport to the Southern Ocean (obtained from the time-delayed and scaled oceanic subsurface warming in CMIP5 models in relation to the global mean surface warming), and the observed range of responses of basal ice shelf melting to oceanic warming outside the ice shelf cavity. This uncertainty in basal ice shelf melting is then convoluted with the linear response functions of each of the 16 ice sheet models to obtain the ice flow response to the individual global warming path. The model median for the observational period from 1992 to 2017 of the ice loss due to basal ice shelf melting is 10.mm, with a likely range between 5.2 and 21.3 mm. For the same period the Antarctic ice sheet lost mass equivalent to 7.4 mm of global sea level rise, with a standard deviation of 3.7 mm (Shepherd et al., 2018) including all processes, especially surface-mass-balance changes. For the unabated warming path, Representative Concentration Pathway 8.5 (RCP8.5), we obtain a median contribution of the Antarctic ice sheet to global mean sea level rise from basal ice shelf melting within the 21st century of 17 cm, with a likely range (66th percentile around the mean) between 9 and 36 cm and a very likely range (90th percentile around the mean) between 6 and 5 cm. For the RCP2.6 warming path, which will keep the global mean temperature below 2°C of global warming and is thus consistent with the Paris Climate Agreement, the procedure yields a median of 13 cm of global mean sea level contribution. The likely range for the RCP2.6 scenario is between 7 and 24 cm, and the very likely range is between 4 and 37 cm. The structural uncertainties in the method do not allow for an interpretation of any higher uncertainty percentiles. We provide projections for the five Antarctic regions and for each model and each scenario separately. The rate of sea level contribution is highest under the RCP8.5 scenario. The maximum within the 21st century of the median value is 4 cm per decade, with a likely range between 2 and 9 cm per decade and a very likely range between 1 and 14 cm per decade.

• Research Organization: Lawrence Berkeley National Laboratory (LBNL), Berkeley, CA (United States); Los Alamos National Laboratory (LANL), Los Alamos, NM (United States); Sandia National Lab. (SNL-NM), Albuquerque, NM (United States)
• Sponsoring Organization: USDOE Office of Science (SC), Advanced Scientific Computing Research (ASCR); USDOE Office of Science (SC), Biological and Environmental Research (BER); European Research Council (ERC); Dutch Ministry of Education, Culture and Science; Japan Society for the Promotion of Science (JSPS); German Federal Ministry of Education and Research (BMBF); German Research Foundation (DFG); National Science Foundation (NSF); USDOE Office of Science (SC). Advanced Scientific Computing Research (ASCR) (SC-21)
• Grant/Contract Number: AC02-05CH11231; 610055; 024.002.001; JP16H02224; JP17H06104; JP17H06323; 01LP1511B; LE1448/6-1; LE1448/7-1; 1852977; 89233218CNA000001; NA0003525
• OSTI ID: 1599529
• Alternate ID(s): OSTI ID: 1604738; OSTI ID: 1631571; OSTI ID: 1831173
• Report Number(s): LA-UR-20-20042; SAND-2021-2118J
• Journal Information: Earth System Dynamics (Online), Journal Name: Earth System Dynamics (Online) Vol. 11 Journal Issue: 1; ISSN 2190-4987
• Publisher: Copernicus Publications, EGU
• Country of Publication: Germany
• Language: English

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