Grounding Line Migration through the Calving Season at Jakobshavn Isbræ, Greenland, observed with Terrestrial Radar Interferometry

• Main Authors: Xie, Surui, Dixon, Timothy H., Voytenko, Denis, Deng, Fanghui, Holland, David M.
• Format: Article in Journal/Newspaper
• Language: unknown
• Published: Digital Commons @ University of South Florida 2018
• Subjects: Earth Sciences; Greenland; Jakobshavn Isbræ; glacier; Jakobshavn; Jakobshavn isbræ
• Online Access: https://digitalcommons.usf.edu/geo_facpub/1523; https://digitalcommons.usf.edu/cgi/viewcontent.cgi?article=2502&context=geo_facpub

Ice velocity variations near the terminus of Jakobshavn Isbræ, Greenland, were observed with a terrestrial radar interferometer (TRI) during three summer campaigns in 2012, 2015, and 2016. We estimate a ∼ 1km wide floating zone near the calving front in early summer of 2015 and 2016, where ice moves in phase with ocean tides. Digital elevation models (DEMs) generated by the TRI show that the glacier front here was much thinner (within 1km of the glacier front, average ice surface is ∼ 100 and ∼ 110m above local sea level in 2015 and 2016, respectively) than ice upstream (average ice surface is > 150m above local sea level at 2–3km to the glacier front in 2015 and 2016). However, in late summer 2012, there is no evidence of a floating ice tongue in the TRI observations. Average ice surface elevation near the glacier front was also higher, ∼ 125m above local sea level within 1km of the glacier front. We hypothesize that during Jakobshavn Isbræ's recent calving seasons the ice front advances ∼ 3km from winter to spring, forming a > 1km long floating ice tongue. During the subsequent calving season in mid- and late summer, the glacier retreats by losing its floating portion through a sequence of calving events. By late summer, the entire glacier is likely grounded. In addition to ice velocity variation driven by tides, we also observed a velocity variation in the mélange and floating ice front that is non-parallel to long-term ice flow motion. This cross-flow-line signal is in phase with the first time derivative of tidal height and is likely associated with tidal currents or bed topography.