An ice-sheet-wide framework for englacial attenuation from ice-penetrating radar data

Radar inference of the bulk properties of glacier beds, most notably identifying basal melting, is, in general, derived from the basal reflection coefficient. On the scale of an ice sheet, unambiguous determination of basal reflection is primarily limited by uncertainty in the englacial attenuation...

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Published in:The Cryosphere
Main Authors: Jordan, T. M., Bamber, J. L., Williams, C. N., Paden, J. D., Siegert, M. J., Huybrechts, P., Gagliardini, O., Gillet-Chaulet, F.
Format: Text
Language:English
Published: 2018
Subjects:
Online Access:https://doi.org/10.5194/tc-10-1547-2016
https://tc.copernicus.org/articles/10/1547/2016/
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spelling ftcopernicus:oai:publications.copernicus.org:tc49396 2023-05-15T16:03:05+02:00 An ice-sheet-wide framework for englacial attenuation from ice-penetrating radar data Jordan, T. M. Bamber, J. L. Williams, C. N. Paden, J. D. Siegert, M. J. Huybrechts, P. Gagliardini, O. Gillet-Chaulet, F. 2018-09-27 application/pdf https://doi.org/10.5194/tc-10-1547-2016 https://tc.copernicus.org/articles/10/1547/2016/ eng eng doi:10.5194/tc-10-1547-2016 https://tc.copernicus.org/articles/10/1547/2016/ eISSN: 1994-0424 Text 2018 ftcopernicus https://doi.org/10.5194/tc-10-1547-2016 2020-07-20T16:24:03Z Radar inference of the bulk properties of glacier beds, most notably identifying basal melting, is, in general, derived from the basal reflection coefficient. On the scale of an ice sheet, unambiguous determination of basal reflection is primarily limited by uncertainty in the englacial attenuation of the radio wave, which is an Arrhenius function of temperature. Existing bed-returned power algorithms for deriving attenuation assume that the attenuation rate is regionally constant, which is not feasible at an ice-sheet-wide scale. Here we introduce a new semi-empirical framework for deriving englacial attenuation, and, to demonstrate its efficacy, we apply it to the Greenland Ice Sheet. A central feature is the use of a prior Arrhenius temperature model to estimate the spatial variation in englacial attenuation as a first guess input for the radar algorithm. We demonstrate regions of solution convergence for two input temperature fields and for independently analysed field campaigns. The coverage achieved is a trade-off with uncertainty and we propose that the algorithm can be "tuned" for discrimination of basal melt (attenuation loss uncertainty ∼ 5 dB). This is supported by our physically realistic ( ∼ 20 dB) range for the basal reflection coefficient. Finally, we show that the attenuation solution can be used to predict the temperature bias of thermomechanical ice sheet models and is in agreement with known model temperature biases at the Dye 3 ice core. Text Dye 3 Dye-3 glacier Greenland ice core Ice Sheet Copernicus Publications: E-Journals Greenland The Cryosphere 10 4 1547 1570
institution Open Polar
collection Copernicus Publications: E-Journals
op_collection_id ftcopernicus
language English
description Radar inference of the bulk properties of glacier beds, most notably identifying basal melting, is, in general, derived from the basal reflection coefficient. On the scale of an ice sheet, unambiguous determination of basal reflection is primarily limited by uncertainty in the englacial attenuation of the radio wave, which is an Arrhenius function of temperature. Existing bed-returned power algorithms for deriving attenuation assume that the attenuation rate is regionally constant, which is not feasible at an ice-sheet-wide scale. Here we introduce a new semi-empirical framework for deriving englacial attenuation, and, to demonstrate its efficacy, we apply it to the Greenland Ice Sheet. A central feature is the use of a prior Arrhenius temperature model to estimate the spatial variation in englacial attenuation as a first guess input for the radar algorithm. We demonstrate regions of solution convergence for two input temperature fields and for independently analysed field campaigns. The coverage achieved is a trade-off with uncertainty and we propose that the algorithm can be "tuned" for discrimination of basal melt (attenuation loss uncertainty ∼ 5 dB). This is supported by our physically realistic ( ∼ 20 dB) range for the basal reflection coefficient. Finally, we show that the attenuation solution can be used to predict the temperature bias of thermomechanical ice sheet models and is in agreement with known model temperature biases at the Dye 3 ice core.
format Text
author Jordan, T. M.
Bamber, J. L.
Williams, C. N.
Paden, J. D.
Siegert, M. J.
Huybrechts, P.
Gagliardini, O.
Gillet-Chaulet, F.
spellingShingle Jordan, T. M.
Bamber, J. L.
Williams, C. N.
Paden, J. D.
Siegert, M. J.
Huybrechts, P.
Gagliardini, O.
Gillet-Chaulet, F.
An ice-sheet-wide framework for englacial attenuation from ice-penetrating radar data
author_facet Jordan, T. M.
Bamber, J. L.
Williams, C. N.
Paden, J. D.
Siegert, M. J.
Huybrechts, P.
Gagliardini, O.
Gillet-Chaulet, F.
author_sort Jordan, T. M.
title An ice-sheet-wide framework for englacial attenuation from ice-penetrating radar data
title_short An ice-sheet-wide framework for englacial attenuation from ice-penetrating radar data
title_full An ice-sheet-wide framework for englacial attenuation from ice-penetrating radar data
title_fullStr An ice-sheet-wide framework for englacial attenuation from ice-penetrating radar data
title_full_unstemmed An ice-sheet-wide framework for englacial attenuation from ice-penetrating radar data
title_sort ice-sheet-wide framework for englacial attenuation from ice-penetrating radar data
publishDate 2018
url https://doi.org/10.5194/tc-10-1547-2016
https://tc.copernicus.org/articles/10/1547/2016/
geographic Greenland
geographic_facet Greenland
genre Dye 3
Dye-3
glacier
Greenland
ice core
Ice Sheet
genre_facet Dye 3
Dye-3
glacier
Greenland
ice core
Ice Sheet
op_source eISSN: 1994-0424
op_relation doi:10.5194/tc-10-1547-2016
https://tc.copernicus.org/articles/10/1547/2016/
op_doi https://doi.org/10.5194/tc-10-1547-2016
container_title The Cryosphere
container_volume 10
container_issue 4
container_start_page 1547
op_container_end_page 1570
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