HR: 16:30h
AN: C54A-03 [Abstracts]
TI: Spatial Variation of Basal Conditions on Kamb Ice Stream
AU: * Jacobel, R W
EM: jacobel@stolaf.edu
AF: Department of Physics, St. Olaf College, 1500 St. Olaf Ave., Northfield, MN 55057, United
States
AU: Welch, B C
EM: welchb@stolaf.edu
AF: Department of Physics, St. Olaf College, 1500 St. Olaf Ave., Northfield, MN 55057, United
States
AU: Osterhouse, D
EM: osterhou@stolaf.edu
AF: Department of Physics, St. Olaf College, 1500 St. Olaf Ave., Northfield, MN 55057, United
States
AU: Pettersson, R
EM: rickard.pettersson@geo.uu.se
AF: Department of Earth Sciences, Uppsala University, Villavägen 16,
Uppsala, SE-752 36, Sweden
AU: MacGregor, J A
EM: joemac@ u.washington.edu
AF: Department of Earth and Space Sciences, University of Washington, Johnson Hall 070, Box
351350, Seattle, WA 98195-1310, United States
AB:
Radar profiles of bed echo intensity provide a way to survey conditions at the ice-bed interface and test for the
presence or absence of water. However, extracting information about bed properties from bed echo intensities
requires an estimate of the dielectric attenuation loss through the ice. A recent survey [MacGregor et al., 2007]
found that the few reported values of depth-averaged attenuation rates in West Antarctica vary by a factor of 3,
presumably due to spatial variations in the chemistry and temperature profiles of the ice. Thus, a single value for
depth-averaged ice-sheet attenuation cannot be assumed, even over a relatively small region.
We measured attenuation rates at several locations on and near Kamb Ice Stream (KIS) by examining basal echo
intensity values as a function of ice thickness from constant-offset radar data acquired in 2004-2006. Our values
obtained for Siple Dome of 29 dB/km agree with previous measurements [Gades et al., 2000] and the recent
calculations and model results of MacGregor et al. [2007]. On KIS, we measured attenuation values of 20 dB/km
over the "sticky spot", where ice has become stagnant. This value is
consistent with an attenuation model over the sticky spot calculated using borehole temperature data
[Engelhardt, 2005] and chemistry data from the Siple Dome ice core. Our radar profiles in the main trunk region
of KIS yield a slightly lower value of 15 dB/km, presumably because colder ice is still being advected from inland
West Antarctica.
Using these values of attenuation, we calculated the basal radar reflectivity at the ice-bed
interface in the regions of all our surveys. We found that most regions of the bed in the trunk of KIS have high
basal reflectivities and that these values are similar to those obtained in locations where water was found in the
Caltech boreholes [Engelhardt, 2005]. Areas of lower bed reflectivity are limited to the sticky spot, where a
borehole found a dry bed, and along the margins of KIS. We use these results to hypothesize about the
stagnation of KIS and the possibility of its reactivation.
UR: http://www.stolaf.edu/other/cegsic
DE: 0726 Ice sheets
DE: 0730 Ice streams
DE: 0774 Dynamics
DE: 0776 Glaciology (1621, 1827, 1863)
DE: 0794 Instruments and techniques
SC: Cryosphere [C]
MN: 2007 Fall Meeting