Effect of ice sheet thickness on formation of the Hiawatha impact crater
Introduction
Recently, a putative impact crater with the diameter of km was discovered beneath the Hiawatha Glacier in northwestern Greenland (Fig. 1) (Kjær et al., 2018). The analysis of the glaciofluvial sediment samples collected from the river draining the structure shows the presence of shocked quartz, a marker indicative of meteoritic impact. Further, elevated concentrations of platinum-group elements (PGE) were found in the samples containing shocked quartz, and Kjær et al. (2018) further asserted that the putative impact crater may have been formed by a fairly rare iron asteroid. The size of the crater suggests that its formation likely caused significant regional – and perhaps even global – environmental perturbations (Toon et al., 1997; Erickson et al., 2020). As per scaling laws (Johnson et al., 2016b), to form a 31 km in diameter impact structure, an iron asteroid impacting at 17 km s−1 at an incidence angle of 45° would have to be nearly 2 km wide (Collins et al., 2004). The probability of any composition asteroid of that size hitting Earth is low but non-negligible, occurring once every ∼2 million years (Silber et al., 2018).
One of the major questions concerning the Hiawatha structure is its age. Although material suitable for radiometric dating has not yet been found and analyzed, radiostratigraphic and geomorphologic evidence suggest that the structure most likely was formed after the Pleistocene inception of the Greenland Ice Sheet (Kjær et al., 2018). This tentative conclusion was further supported by identification of impact-heated conifer wood fragments associated with impactite grains from the Hiawatha glaciofluvial outwash that is probably derived from the Early Pleistocene deposits (Garde et al., 2020). So, while the sum of available evidence is suggestive of a geologically young age, no firm evidence of its age yet exists.
Confirmed impact craters generally contain shock-diagnostic materials, such as extensive fracturing and brecciation, high-pressure minerals, and planar deformation features (PDFs) in quartz. Younger craters generally exhibit well-defined morphologic features and are less degraded than older impact structures (French and Koeberl, 2010; Melosh, 1989). For example, fresh craters feature relatively sharp and raised rims with overturned stratigraphy, and the lack of disrupted features (French and Koeberl, 2010; Melosh, 1989). Based on these identifiers, the putative Hiawatha impact structure might be relatively fresh. It has a rim-to-floor depth of m, and a dissected central uplift that is up to 50 m high and whose peaks are up to ∼8 km apart (Kjær et al., 2018). For a subaerial impact (no ice present), simple modeling suggests that a fresh, 31 km-diameter subaerial crater would display a peak ring (Pike, 1985) and have a rim-to-floor depth of ∼830 m (Collins et al., 2005). So, Hiawatha's morphology is muted compared to that expected for a subaerial impact, and yet it retains fundamental elements of a crater morphology (Fig. 1). One would also expect an impact of this size would blanket Greenland in rocky ejecta. If the impact occurred in the late Pleistocene, it is generally assumed that such ejecta should be easily identifiable within the six existing deep ice cores that typically record most of Last Glacial Period (115–11.7 ka) to the present day, including the Bølling-Allerød and the Younger Dryas (YD) transitions (Kjær et al., 2018). The YD is the millennium-long cold period that followed the Bølling-Allerød interstadial near the end of the last ice age at ∼12.8 ka. Although there is a Pt anomaly of possible cosmic origin at the Bølling-Allerød/YD boundary in the Greenland Ice Sheet Project 2 (GISP2) ice core (Petaev et al., 2013), there is no other evidence of rocky ejecta in any ice cores (Seo et al., 2019) and substantial evidence challenging an impact that time (e.g., Sun et al., 2020). The presence of ice, however, would affect the morphology and depth of the final crater, as well as the distribution of rocky ejecta (Senft and Stewart, 2008).
Here we model several possible scenarios for the formation of the putative Hiawatha impact crater using the iSALE-2D shock physics code (Collins et al., 2004; Wünnemann et al., 2006). To understand the effect of a pre-impact ice sheet, we investigate how the presence of thick ice affects the crater morphology and the dynamics and placement of the distal ejecta blanket.
Section snippets
Methods
We model the formation of the putative Hiawatha impact crater using the iSALE-2D Eulerian shock physics code (Collins et al., 2004; Ivanov et al., 1997; Melosh et al., 1992; Wünnemann et al., 2006), which is based on the SALE (Simplified Arbitrary Lagrangian Eulerian) hydrocode solution algorithm (Amsden et al., 1980). This hydrocode has been used previously to model impacts on Earth and other planetary bodies, and its outputs compare well against laboratory experiments (e.g., Bray et al., 2014
Results and discussion
In this section, we describe the effect of ice thickness on crater morphology and distal rocky ejecta. The final crater diameter produced in all simulations is approximately 31 km, consistent with the putative Hiawatha impact structure.
Conclusions
The recent discovery of the putative 31 km-wide Hiawatha impact crater beneath the Greenland Ice Sheet reinvigorated interest in ice-affected impact processes (Kjær et al., 2018). We used iSALE-2D shock physics code to model possible formation scenarios for this putative impact crater and investigate the resulting morphology and the emplacement of distal rocky ejecta to infer possible conditions at the time of crater formation. The morphology of the simulated crater is qualitatively consistent
Credit authorship contribution statement
EAS, EB and BCJ performed numerical modeling. EAS wrote majority of the manuscript. JAM and NKL contributed with the expertise on the area and maps figures. WES contributed with interpretation. All authors contributed to writing the paper.
Declaration of Competing Interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
Acknowledgments
We gratefully acknowledge the developers of iSALE-2D (www.isale-code.de), the simulation code used in this work, including Gareth Collins, Kai Wünnermann, Dirk Elbeshausen, Boris Ivanov and Jay Melosh. Some plots in this work were created with the pySALEPlot tool written by Tom Davison. All data associated with this study are listed in tables in the supporting information and shown in figures. The simulations were performed using iSALE-2D, version Dellen r-2114. The simulation inputs and model
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