Deriving micro- to macro-scale seismic velocities from ice-core c axis orientations

<p><strong>Abstract.</strong> One of the great challenges in glaciology is the ability to estimate the bulk ice anisotropy in ice sheets and glaciers, which is needed to improve our understanding of ice-sheet dynamics. We investigate the effect of crystal anisotropy on seismic velo...

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Hauptverfasser: Kerch, Johanna (VerfasserIn) , Diez, Anja (VerfasserIn) , Weikusat, Ilka (VerfasserIn) , Eisen, Olaf (VerfasserIn)
Dokumenttyp: Article (Journal)
Sprache:Englisch
Veröffentlicht: 23 May 2018
In: The Cryosphere
Year: 2018, Jahrgang: 12, Heft: 5, Pages: 1715-1734
ISSN:1994-0424
DOI:https://doi.org/10.5194/tc-12-1715-2018
Online-Zugang:Verlag, Volltext: https://doi.org/https://doi.org/10.5194/tc-12-1715-2018
Verlag, Volltext: https://www.the-cryosphere.net/12/1715/2018/
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Verfasserangaben:Johanna Kerch, Anja Diez, Ilka Weikusat, and Olaf Eisen

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520 |a <p><strong>Abstract.</strong> One of the great challenges in glaciology is the ability to estimate the bulk ice anisotropy in ice sheets and glaciers, which is needed to improve our understanding of ice-sheet dynamics. We investigate the effect of crystal anisotropy on seismic velocities in glacier ice and revisit the framework which is based on fabric eigenvalues to derive approximate seismic velocities by exploiting the assumed symmetry. In contrast to previous studies, we calculate the seismic velocities using the exact <i>c</i> axis angles describing the orientations of the crystal ensemble in an ice-core sample. We apply this approach to fabric data sets from an alpine and a polar ice core. Our results provide a quantitative evaluation of the earlier approximative eigenvalue framework. For near-vertical incidence our results differ by up to 135 m s<sup>−1</sup> for P-wave and 200 m s<sup>−1</sup> for S-wave velocity compared to the earlier framework (estimated 1 % difference in average P-wave velocity at the bedrock for the short alpine ice core). We quantify the influence of shear-wave splitting at the bedrock as 45 m s<sup>−1</sup> for the alpine ice core and 59 m s<sup>−1</sup> for the polar ice core. At non-vertical incidence we obtain differences of up to 185 m s<sup>−1</sup> for P-wave and 280 m s<sup>−1</sup> for S-wave velocities. Additionally, our findings highlight the variation in seismic velocity at non-vertical incidence as a function of the horizontal azimuth of the seismic plane, which can be significant for non-symmetric orientation distributions and results in a strong azimuth-dependent shear-wave splitting of max. 281 m s<sup>−1</sup> at some depths. For a given incidence angle and depth we estimated changes in phase velocity of almost 200 m s<sup>−1</sup> for P wave and more than 200 m s<sup>−1</sup> for S wave and shear-wave splitting under a rotating seismic plane. We assess for the first time the change in seismic anisotropy that can be expected on a short spatial (vertical) scale in a glacier due to strong variability in crystal-orientation fabric (±50 m s<sup>−1</sup> per 10 cm). Our investigation of seismic anisotropy based on ice-core data contributes to advancing the interpretation of seismic data, with respect to extracting bulk information about crystal anisotropy, without having to drill an ice core and with special regard to future applications employing ultrasonic sounding.</p> 
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