SMITH and Reference Smith and EvansEvans (1972) consider reflections of radio waves from a layer of brine-soaked firn in their discussion of absorption by water inclusions. I would like to report on some measurements made on the ice shelf near McMurdo station (Reference Clough and BentleyClough and Bentley, 1967).
Profiling from the surface was carried out over 100 km of the grid system partially shown in Figure 1. Toward the western end of the shelf an abrupt change in apparent thickness was observed. On the western side, the depth to the reflector was about 32–45 m compared with 95–120 m on the eastern side. The shallow reflector can be attributed to a brine penetration layer while the greater depth is consistent with the thickness of the ice shelf measured elsewhere.
Brine-soaked firn was found at a depth of 19 m in cores taken near station 207 (Reference HeineHeine, 1968), and at 26 m midway between stations 207 and 320 (personal communication from A. J. Heine in 1972). The eastern extent of brine penetration was found, by radio echo profiling, about 5.5 km east of 207 where the depth to the brine layer was about 32 m. The depth corresponds well with Heine’s estimate of 30–31 m at station 320 (personal communication from A. J. Heine in 1972). A portion of the boundary delineating the extent of brine penetration into the ice shelf was mapped by a zig-zag traverse. The boundary and traverse crossing points are shown in Figure 1.
Reflection records obtained in the vicinity of the boundary are shown in Figure 2. The recorded echo changed completely from deep to shallow over distances of a few meters. Moving a few meters further to either side of the boundary normally resulted in extinction of the weak echo seen in Figure 2a or c. A very high reflection coefficient at the top of the brine layer and strong absorption within the layer result in no observed reflection from the bottom of the ice shelf in the region of the brine layer. The two echoes in Figure 2b occur when both reflectors are “illuminated” by the transmitted wave. The time shift to the brine layer as seen in Figure 2b and c may be due to the shape of the brine layer edge as well as to oblique incidence of the wave.
This research was supported by NSF Grant GA552.