Jökull


Jökull - 01.01.2021, Page 61

Jökull - 01.01.2021, Page 61
Bedrock and tephra layer topography within the Katla caldera of the magenta coloured points in Figure 5c, denoting bed interpreted from the 2D migrated profile, more than 80 m below the bed derived from the 3D migrated data; generally the 2D migrated traces are above the 3D migrated DEM due to cross-track reflections. This was due to wrong interpretation of bed reflection in the 2D migrated data. The first strong reflection near the bed in the 2D migrated profiles was considered to be a reflection from the top of a water chamber di- rectly beneath the centre of K6. A reflection at greater depth, considered to be from the bed directly beneath, was in this case likely a strong cross-track reflection from a mound 300 m NNE of this location. The actual bed directly beneath the radar was probably screened by the water body in spring 2016. This comparison demonstrates that using 2D mi- grated RES-data, without any adjustments to compen- sate for the effects of cross track reflections, will re- sult in an upward bias of the resulting bed DEM for steep and rugged bed terrain. The 10 m offset of 2D migrated RES-data for this area is too high to be explained by other systematic errors. Accurately repeated surveys, both the 3D migrated surveys pre- sented here and repeated 2D migrated profiles sur- veyed on Mýrdalsjökull and Vatnajökull (Magnússon et al., 2017; 2021) suggest that temporal variations due to such errors are generally less than 3 m from one survey to another. A similar experiment comparing 2D and 3D migrated RES-data obtained above steep bedrock beneath Gulkana Glacier, Alaska, also indi- cated a similar underestimate in bed elevation from the 2D migrated data (Moran et al., 2000). The com- parison presented here also shows that if the effects of cross track reflections are not considered, measuring a denser set of profiles than done in 2016 for K6 and vicinity (∼200 m between profiles) would not have much increased the accuracy of the interpolated DEM. The DEM accuracy had already reached the accuracy of the input data used in the interpolation. This sug- gests that the interpolation errors were insignificant in comparison with the errors caused by the limitations of the 2D migration. The benefit of profiles denser than 200 m apart for similar radar set-ups in areas of comparable bed slopes and ice thickness (300–600 m) are likely small if the effects of cross track reflections are not considered. For more gentle slopes, denser profiles can improve the resulting bedrock DEM. In our study, the difference at the crossing points of the 2D migrated profiles has been used to adjust the location of traced bed reflections for the profiles that are likely to be substantially affected by cross-track reflections, before carrying out the bedrock interpola- tion (see Data and Methods and Figure 3). We expect our simple approach to substantially reduce the errors caused by cross-track reflections, but we still expect significant errors of this kind to remain in our bedrock DEM in steep areas. Water potential and drainage basins Using the new bedrock DEM and the surface DEM from 2019, with 20× 20m cell size, the water divides between drainage basins (Figure 7b) were updated from previous work (Björnsson et al., 2000, and more recent unpublished work of IES-glaciology group) within the study area. This was done by assuming that the water flow along the gradient of the static wa- ter potential, ϕ, at the glacier bed with water pressure corresponding to the full ice overburden pressure (e.g. Björnsson, 1975): ϕ=ρwgzb + ρigH Eq. 1 where ρw=1000 kg m−3 and ρi=900 kg m−3 is the density of water and ice, g=9.82 m s−2 the accel- eration due to gravity and zb the bedrock elevation. H = zs−zb is the ice thickness where zs is the surface elevation. The procedure of drawing water divides, as explained in Magnússon et al. (2012), includes fil- tering of the surface DEM with a circular filter prior to calculating the water potential. The filter weight decreases linearly to zero at distances corresponding to half ice-thickness, hence it is assumed that due to the strength of the ice, the weight of an ice column affects the ice overburden pressure over a distance equal to the ice thickness. The filter smooths out noise and small scale errors in the DEM as well as actual small scale features such as crevasses. The revision of the water divides (Figure 7b) shifts them in some cases a few hundred metres from the ones presented by Björnsson et al. (2000). Substantial part of this change is not related to the improved bedrock DEM but to difference between surface DEMs; the change JÖKULL No. 71, 2021 59
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