日本地球惑星科学連合2019年大会

講演情報

[J] 口頭発表

セッション記号 M (領域外・複数領域) » M-IS ジョイント

[M-IS14] 南大洋・南極氷床が駆動する全球気候変動

2019年5月27日(月) 10:45 〜 12:15 コンベンションホールB (2F)

コンビーナ:関 宰(北海道大学低温科学研究所)、岡 顕(東京大学大気海洋研究所)、植村 立(琉球大学 理学部)、真壁 竜介(国立極地研究所)、座長:シェリフ多田野 サム(東京大学)

11:30 〜 11:45

[MIS14-09] Vertical ice flow motions obtained from year-round GNSS observations on Shirase Glacier, Antarctica

*青山 雄一1,2土井 浩一郎1,2平野 大輔3田村 岳史1,2青木 茂3渋谷 和雄1 (1.国立極地研究所、2.総合研究大学院大学、3.北海道大学低温科学研究所)

キーワード:白瀬氷河上でのGNSS通年観測、アクセスが困難な場所での無人観測

The Antarctic ice sheet is a huge heat sink acting as a feedback controller for adjusting global warming, so a loss of its mass would cause a great impact on the global climate change. It is valuable to evaluate an Antarctic ice mass balance, which is a consequence of competition between an ice discharge and a snow accumulation. With an objective of estimating the ice discharge around Lützow-Holmbukta, East Antarctica, we have measured three-dimensional (3D) ice flow motions around a grounding line of Shirase Glacier, which is fastest and largest ice stream in Lützow-Holmbukta.

We first performed one-month GPS measurement near the calving front of Shirase Glacier in 2011/2012 austral summer. The three-dimensional position of this site was determined by the kinematic precise point positioning (kPPP) method at every 30 seconds with a 4-5-cm precision for 25 days. From the 30-s interval position, we estimated the ice flow velocity vector, the basal melting rate of the iceberg, and ocean tidal variations (Aoyama et al. 2016). Subsequently, a year-round GNSS measurement system was installed six kilometers downstream from the grounding line of Shirase Glacier at the end of Jan. 2015. By maintaining this year-round system (changing SD card and battery) every austral summer season, we have already obtained a three-years continuous data from Jan. 30, 2015 to Dec. 30, 2017.
We analyzed the time series of the three-dimensional position of this system with kPPP method. The time series revealed the ice flow motion downstream from the grounding line of Shirase Glacier during 2015-2017. Focusing on the vertical motion, there is no remarkable ocean tidal variation. And the obtained vertical flow motion shows gradually descent, then rise, again descent slope. In order to clarify whether such vertical change is local or wide area, we compared with a TanDEM-X 90m DEM (Rizzoli et al., 2017). In the presentation, we will show properties of the ice flow motion downstream the grounding line of Shirase Glacier.