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1 <p>Today, <a href="mailto:[email protected]">Indraneel | |
2 Kasmalkar</a> had his paper published in <a | |
3 href="https://agupubs.onlinelibrary.wiley.com/journal/19422466">Journal … | |
4 Geophysical Research: Earth Surface</a>. Congratulations Neel! He used | |
5 my software <a href="https://src.adamsgaard.dk/sphere">sphere</a>, and | |
6 sheared a granular assembledge with a non-trivial forcing in order to | |
7 learn more about subglacial sediment behavior.</p> | |
8 | |
9 <p>Here's an example visualization from the study:</p> | |
10 <center> | |
11 <video poster="video/neel.jpg" | |
12 controls preload="none" class="mediaframe"> | |
13 <source src="video/neel.mp4" type="video/mp4"> | |
14 <a href="video/neel.mp4">Link</a> | |
15 </video> | |
16 </center> | |
17 | |
18 <h2>Abstract</h2> | |
19 <blockquote> | |
20 <b>Shear Variation at the Ice-Till Interface Changes the Spatial | |
21 Distribution of Till Porosity and Meltwater Drainage</b> | |
22 <br><br> | |
23 Indraneel Kasmalkar(1), Anders Damsgaard(2), Liran Goren(3), Jenny Sucka… | |
24 <br><br> | |
25 1: Department of Computational and Mathematical Engineering, Stanford Un… | |
26 <br> | |
27 2: Department of Geoscience, Aarhus University, Denmark | |
28 <br> | |
29 3: Department of Earth and Environmental Sciences, Ben-Gurion University… | |
30 <br> | |
31 4: Department of Geophysics, Stanford University, CA, USA | |
32 <br> | |
33 5: Department of Civil and Environmental Engineering, Stanford Universit… | |
34 <br><br> | |
35 Plain-language summary:<br> | |
36 The ice at the base of certain glaciers moves over soft sediments | |
37 that route meltwater through the pore spaces in between the sediment | |
38 grains. The ice shears the sediment, but it is not clear if this slow | |
39 shearing is capable of changing the structure or volume of the pore spac… | |
40 or the path of the meltwater that flows through the sediment. To study | |
41 the relations between the shearing of the sediment and the changes in its | |
42 pore space, we use computer simulations that portray the sediment as a | |
43 collection of closely packed spherical grains, where the pores are filled | |
44 with meltwater. To shear the simulated sediment, the grains at the top | |
45 are pushed with fixed speeds in the horizontal direction. Despite the | |
46 slow shear, which is generally thought of as having no effect on pore | |
47 space, our results show that shearing changes the sizes of the pores | |
48 in between the grains, where large pores are formed near the top of the | |
49 sediment layer. If the grains at the top are pushed with uneven speeds, | |
50 then the largest pores are formed in the areas where grain speeds vary | |
51 the most. We show that the exchange of meltwater between neighboring | |
52 pores is faster than the movement of the grains, indicating that the | |
53 meltwater can adjust quickly to changing pore space. | |
54 <br><br> | |
55 Abstract:<br> | |
56 Many subglacial environments consist of a fine-grained, deformable | |
57 sediment bed, known as till, hosting an active hydrological system that | |
58 routes meltwater. Observations show that the till undergoes substantial | |
59 shear deformation as a result of the motion of the overlying ice. The | |
60 deformation of the till, coupled with the dynamics of the hydrological | |
61 system, is further affected by the substantial strain rate variability | |
62 in subglacial conditions resulting from spatial heterogeneity at the | |
63 bed. However, it is not clear if the relatively low magnitudes of strain | |
64 rates affect the bed structure or its hydrology. We study how laterally | |
65 varying shear along the ice-bed interface alters sediment porosity and | |
66 affects the flux of meltwater through the pore spaces. We use a discrete | |
67 element model consisting of a collection of spherical, elasto-frictional | |
68 grains with water-saturated pore spaces to simulate the deformation | |
69 of the granular bed. Our results show that a deforming granular layer | |
70 exhibits substantial spatial variability in porosity in the pseudo-static | |
71 shear regime, where shear strain rates are relatively low. In particular, | |
72 laterally varying shear at the shearing interface creates a narrow zone | |
73 of elevated porosity which has increased susceptibility to plastic | |
74 failure. Despite the changes in porosity, our analysis suggests that | |
75 the pore pressure equilibrates near-instantaneously relative to the | |
76 deformation at critical state, inhibiting potential strain rate dependen… | |
77 of the deformation caused by bed hardening or weakening resulting from | |
78 pore pressure changes. We relate shear variation to porosity evolution | |
79 and drainage element formation in actively deforming subglacial tills. | |
80 </blockquote> | |
81 | |
82 <h2>Links and references:</h2> | |
83 <ul> | |
84 <li><a href="https://doi.org/10.1029/2021JF006460">Publication o… | |
85 <li><a href="papers/Kasmalkar et al 2021 Shear variation at the … | |
86 <li><a href="https://src.adamsgaard.dk/sphere">Simulation softwa… | |
87 </ul> |