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A ground-based radar backscatter investigation in the percolation zone of the Greenland ice sheet

机译:格陵兰冰原渗流区的地面雷达反向散射调查

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Satellite radar altimeters and scatterometers deployed over ice sheets experience backscatter from the surface and from within the snowpack, termed surface and volume backscatter respectively. In order to assess the errors in satellite altimeter measurements it is vital to know where the return is originating from in the snowpack. This return can vary spatially and temporally. Seasonal variations in the volume backscatter can be a major complicating factor in the radar return from the percolation zone. Ground-based step-frequency radar was deployed in the percolation zone of the Greenland Ice Sheet at ~ 1945 m elevation (69 51N, 47 15W), Previous measurements in this area made by scientists from the Byrd Polar Research Centre and the University of Kansas, undertaken prior to summer melt events, have shown the strongest backscatter from ice features at around 1 m depth buried beneath the previous end-of-summer surface. In autumn 2004, radar measurements in the Ku band with bandwidths of 1 and 8 GHz were made alongside detailed stratigraphic observations within a 1 km{sup}2 site. The radar results revealed no continuous reflecting horizons in the upper 3.5 m of the firn. Shallow cores and snowpits also indicated that there were no spatially continuous stratigraphic horizons across the study site. An average electromagnetic wave velocity of 2.11 ± 0.05 × 10{sup}8 m s{sup}(-1) was determined for the upper metre of the firn. Surface and volume backscatter at vertical incidence were calculated using a standard model. The contribution of the surface backscatter to the total backscatter was on average 6 dB higher than that of the volume backscatter. However, at the higher 8 GHz bandwidth the strongest return frequently originated not from the surface but from within the upper 30 cm of the snowpack, most probably from thin ice layers. At 1 GHz bandwidth these ice layers were not always resolved; their return merged with the surface return, causing it to broaden, with the peak and leading edge moving down. Modelling using density and thickness measurements from shallow cores and snowpits showed that the backscatter from these shallow, thin ice layers could be stronger than the surface return owing to constructive interference from the top and base of the layers.
机译:部署在冰盖上的卫星雷达高度计和散射仪经历了从地面和积雪内部的反向散射,分别称为表面和体积反向散射。为了评估卫星高度计测量中的误差,至关重要的是要知道返回的来源是雪堆。该收益可以在空间和时间上变化。体积反向散射的季节性变化可能是雷达从渗流区返回的主要复杂因素。地面步频雷达被部署在格陵兰冰原的渗流区,海拔约1945 m(69 51N,47 15W),该区域以前的测量是由伯德极地研究中心和堪萨斯大学进行的在夏季融化事件之前进行的观测表明,埋藏在先前夏末表面下方约1 m深度处的冰层特征产生的最强反向散射。 2004年秋天,在1 km {sup} 2站点内,在Ku频段进行了带宽为1和8 GHz的雷达测量以及详细的地层观测。雷达结果表明,在机舱上方3.5 m处没有连续的反射层。浅层岩心和积雪坑也表明整个研究地点没有空间连续的地层。测得的火星上部米的平均电磁波速度为2.11±0.05×10 {sup} 8 m s {sup}(-1)。使用标准模型计算垂直入射时的表面和体积反向散射。表面反向散射对总反向散射的贡献平均比体积反向散射高6 dB。但是,在较高的8 GHz带宽下,最强的返回频率通常不是来自地面,而是来自雪堆的上部30 cm以内,最有可能来自薄冰层。在1 GHz带宽下,这些冰层并不总是能够解决。他们的收益与表面收益合并,导致其扩大,峰值和前沿下降。使用来自浅层岩心和雪坑的密度和厚度测量结果进行的建模表明,由于这些层的顶部和底部的相长干涉,这些浅层,薄层冰层的反向散射可能比表面返回强。

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