日本地球惑星科学連合2019年大会

講演情報

[E] ポスター発表

セッション記号 M (領域外・複数領域) » M-TT 計測技術・研究手法

[M-TT46] 統合地球観測システムとしてのGPS/GNSSの新展開

2019年5月27日(月) 17:15 〜 18:30 ポスター会場 (幕張メッセ国際展示場 8ホール)

コンビーナ:小司 禎教(気象研究所気象衛星・観測システム研究部第2研究室)、市川 香(九州大学応用力学研究所)、太田 雄策(東北大学大学院理学研究科附属地震・噴火予知研究観測センター)、津川 卓也(情報通信研究機構)

[MTT46-P03] 静止衛星によるGNSS-R海面高度計測

*市川 香1奥村 立樹2根田 昌典3馬場 康之4 (1.九州大学応用力学研究所、2.九州大学総合理工学府大気海洋環境システム学専攻、3.京都大学大学院理学研究科、4.京都大学防災研究所)

キーワード:GNSS-R、海面高度計、BeiDou静止GNSS衛星

The GNSS reflectometry (GNSS-R) uses GNSS signals reflected at the sea surface, which are usually eliminated as the multipath error. The reflected GNSS path received at an antenna is always longer than the direct path, so that the height of the antenna from the sea surface is geometrically determined from the excess path length. The excess path length can be either directly determined by measuring the temporal delay of the reflected signals, or indirectly estimated from interferometric cyclic modulations of the received power (often referred as signal-to-noise ratio; SNR) induced by phase differences between the direct and reflected GNSS signals. In the latter method, as the elevation angle of an earth orbiting GNSS satellite changes in time, the geometric reflection point on the sea surface temporally displaces, which results in interferometric changes of the path length during a period while the satellite is in sight. Meanwhile, for a geostationary satellite in BeiDou constellations that are always in sight, the path length changes not by the movement of the satellite but the elevation of the reflection surface, i.e. the sea level rise. In this study, we used the three-month time series (2016/09-11) of the 1Hz SNR of the geostationary BeiDou #02 satellite observed by a GNSS-R system deployed to the Shirahama Oceanographic Observatory Tower owned by Kyoto University (33deg, 42’32’’N, 135deg, 19’58’’E) at the height of ~20m. The geostationary GNSS-R altimetry observed significant flood tides when the wind speed is stably low; the 0.6m sea level rise was successfully determined by the SNR interferometry with 0.05m rms difference. However, significant interferometric SNR changes by tides were not recorded at high or low tides since at least 0.25m sea level change is required for the interferometry cycle. Consequently, the cyclic periods of the geostationary GNSS-R altimetry for tides become long (1-4 hours for 0.25m change in Shirahama), the interferometric variations were usually contaminated by SNR changes induced by the other factors such as winds. On the contrary, faster sea level changes by wave motions could be recognized by the geostationary GNSS-R altimetry, although the temporal sampling intervals of the present data were not adequate.