| Literature DB >> 36151072 |
Aslak Grinsted1, Christine S Hvidberg2, David A Lilien3, Nicholas M Rathmann2, Nanna B Karlsson4, Tamara Gerber2, Helle Astrid Kjær2, Paul Vallelonga5, Dorthe Dahl-Jensen2,3.
Abstract
Mass loss near the ice-sheet margin is evident from remote sensing as frontal retreat and increases in ice velocities. Velocities in the ice sheet interior are orders of magnitude smaller, making it challenging to detect velocity change. Here, we analyze a 35-year record of remotely sensed velocities, and a 6-year record of repeated GPS observations, at the East Greenland Ice-core Project (EastGRIP), located in the middle of the Northeast-Greenland Ice Stream (NEGIS). We find that the shear margins of NEGIS are accelerating, indicating a widening of the ice stream. We demonstrate that the widening of the ice stream is unlikely to be a response to recent changes at the outlets of NEGIS. Modelling indicates that the observed spatial fingerprint of acceleration is more consistent with a softening of the shear margin, e.g. due to evolving fabric or temperature, than a response to external forcing at the surface or bed.Entities:
Year: 2022 PMID: 36151072 PMCID: PMC9508143 DOI: 10.1038/s41467-022-32999-2
Source DB: PubMed Journal: Nat Commun ISSN: 2041-1723 Impact factor: 17.694
Fig. 1Along flow ice acceleration in North–East Greenland based on 1985–2018 velocity data.
Box near EGRIP indicates location of the stake network in Fig. 2. Grid points with less than 10 years of data has been disregarded. The shear margins of the interior are accelerating, indicating that the ice stream is widening. Dashed line shows region of no clear pattern of acceleration separating inland change from frontal changes. Inset shows overview map colored by ice velocity[29].
Fig. 2GPS observations of stakes at EastGRIP show accelerating ice flow.
Background map shows ice velocities[29] draped over the landscape. Arrows indicate the velocity and flow direction of each stake. Sphere colors show the estimated acceleration at each stake where it exceeds 1σ (uncertainties shown in online methods Fig. S2).