2015
DOI: 10.1017/jfm.2015.503
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A boundary layer model for ice stream margins

Abstract: International audienceThe majority of Antarctic ice is discharged via long and narrow fast-flowing ice streams. At ice stream margins, the rapid transition from the vertical shearing flow in the ice ridges surrounding the stream to a rapidly sliding plug flow in the stream itself leads to high stress concentrations and a velocity field whose form is non-trivial to determine. In this paper, we develop a boundary layer theory for this narrow region separating a lubrication-type ice ridge flow and a membrane-type… Show more

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Cited by 28 publications
(99 citation statements)
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References 54 publications
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“…However, if we instead considered a flow line through the shear margin (though this in conflict with other assumptions made in model formulation), then lateral shear heating is non-negligible (10 %). Nonetheless, in order to draw definitive conclusions about specific ice streams, more complete 3-D ice-stream modeling is needed, which takes into account variations in bed properties simulated in this study and also details not captured by a flow-line model, such as fully dynamic ice shelf buttressing, cross-stream variations in basal topography, lateral advection and shear margin migration (Haseloff et al, 2015).…”
Section: Discussionmentioning
confidence: 99%
“…However, if we instead considered a flow line through the shear margin (though this in conflict with other assumptions made in model formulation), then lateral shear heating is non-negligible (10 %). Nonetheless, in order to draw definitive conclusions about specific ice streams, more complete 3-D ice-stream modeling is needed, which takes into account variations in bed properties simulated in this study and also details not captured by a flow-line model, such as fully dynamic ice shelf buttressing, cross-stream variations in basal topography, lateral advection and shear margin migration (Haseloff et al, 2015).…”
Section: Discussionmentioning
confidence: 99%
“…Since we only model processes in the y-z plane, we cannot model the emergence of ice streams and ice ridges, as, for example, in Kyrke-Smith et al (2014). Instead, we assume the existence of an ice stream and adopt the following approximate profile for the ice thickness H (Haseloff et al, 2015):…”
Section: The Modelmentioning
confidence: 99%
“…Models linking the basal yield stress to physical processes can be divided into two categories. In the first, τ c is a function of temperature, in which case the transition from slip to no slip is linked to a transition from a temperate to a frozen bed (Haseloff et al, , ; Jacobson & Raymond, ; Schoof, ). In the second, τ c is a function of the water pressure in the subglacial sediment, in which case the transition from slip to no slip is hydrologically controlled (Elsworth & Suckale, ; Kyrke‐Smith et al, , ; Meyer et al, ; Perol et al, ; Platt et al, ).…”
Section: Introductionmentioning
confidence: 99%
“…The hydrology includes thin-film and channel drainage systems (after Creyts & Schoof, 2009;Hewitt, 2011Hewitt, , 2013. R-channel = Röthlisberger channel. ice streams rely in part on the inflow of ice from the surrounding cold ridges, suppressing the formation of temperate ice (Haseloff et al, 2015;Suckale et al, 2014). Thus, the existence and thickness of a temperate zone must vary along the margin (Figure 1).…”
Section: Introductionmentioning
confidence: 99%