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What drives large-scale glacier detachments? Insights from Flat
Creek Glacier, St. Elias Mountains, Alaska
Mylène Jacquemart1, Michael Loso2, Matthias Leopold3, Ethan Welty4, Etienne Berthier5, Jasmine
S. S. Hansen1, John Sykes6, Kristy Tiampo1
1 Department of Geological Sciences & CIRES, University of Colorado, Boulder, CO, 80309, USA
2 Wrangell-St. Elias National Park and Preserve, Copper Center, AK 99573
3 UWA-School of Agriculture and Environment, University of Western Australia, Perth, 6009, Australia
4 INSTAAR, University of Colorado, Boulder, CO, 80309, USA
5 LEGOS, Université de Toulouse, 31400 Toulouse, France
6 Department of Geography, Simon Fraser University, Burnaby, BC V5A 1S6, Canada
ABSTRACT
Two large-scale glacier detachments occurred at the peaks of the 2013 and 2015 melt seasons, releasing a
cumulative 24.4 – 31.3 x 106 m3 of ice and lithic material from Flat Creek Glacier, St. Elias Mountains,
Alaska. Both events produced highly mobile and destructive flows with runout distances of more than 11
km. Our results suggest that four main factors led to the initial detachment in 2013: Abnormally high
meltwater input, an easily erodible glacier bed, inefficient subglacial drainage due to a cold-ice tongue,
and increased driving stresses stemming from an internal redistribution of ice after 2011. Under a
drastically altered stress regime, the stability of the glacier remained sensitive to water inputs thereafter,
culminating in a second detachment in 2015. The similarities with two large detachments in the Aru
mountains of Tibet suggest that these detachments were caused by a common mechanism, driven by
unusually high meltwater inputs. As meltwater production increases with rising temperatures, the possible
increase in frequency of glacier detachments has direct implications for risk management in glaciated
regions.
INTRODUCTION
Large-scale glacier detachments occur when large portions of valley glaciers’ tongues decouple from the
glacier bed, resulting in catastrophic mass flows (Evans & Delaney, 2015). Recent observations from
around the world – including the 2002 detachment of Kolka Glacier (100–130 x 106 m3; Haeberli et al.,
2004; Evans et al., 2009), the twin 2016 detachments of the Aru glaciers in Tibet (68 x 106 m3 and 83 x
106 m3, respectively; Kääb et al., 2018), the 2007 detachment of Leñas Glacier in the Argentinian Andes
(4 x 106 m3, Falaschi et al., 2019), and repeated ice detachments from an unnamed glacier in central
China (unknown volume; Paul, 2019) – raise the question whether anthropogenic climate change is not
only accelerating glacier retreat, but also introducing a previously unobserved yet catastrophic mechanism
of glacier destruction.
We extend the list above by documenting two large-scale detachments at Flat Creek Glacier,
Alaska, which occurred in 2013 and 2015. Understanding the cause of these hazardous events is critical to
predicting where else they are likely to occur. Although Gilbert et al. (2018) have proposed that the Aru
and Kolka detachments were ultimately caused by a failure of the subglacial till, the climatic and glacial
conditions leading up to these detachments differed significantly (Gilbert et al., 2018, Evans et al., 2009).
In this study, we used data from two field campaigns and a remote sensing analysis to characterize the
geologic, glacial, thermal, and meteorological conditions that led to the Flat Creek detachments. In an
attempt to identify common drivers of glacier detachments, we describe and quantify the Flat Creek
detachments and compare them to those of Aru and Kolka.
STUDY AREA
Prior to the 2013 detachment, informally-named Flat Creek Glacier covered 2.6 km2 (6.5%) of the Flat
Creek watershed (Fig. 1). It occupied a central trough at 2030 – 2650 m above sea level (asl) on the NNE-
facing headwall. Meltwater from the glacier drains into the White River at 1050 m asl. The glacier lies in
a subarctic climate in the rain shadow of the St. Elias Mountains. Over the last decade, the Chisana
weather station (50 km NW of Flat Creek, at 1012 m asl) recorded a mean annual air temperature of -4.5
°C and a mean annual precipitation of 335 mm. Regional and global maps (Jorgenson et al., 2008;
Gruber, 2012), electrical resistivity tomography, and ground temperature measurements (see methods
suppl.) indicate that permafrost is continuous in the upper part of the valley (above 1800 m asl) and
discontinuous-to-sparse on the alluvial fan (below 1600 m asl). Many glaciers in the area have a history of
surging (Post, 1969), and one glacier adjacent to Flat Creek surged between 2012 and 2015. Crosscutting
upper Flat Creek, the influence of the Totschunda Fault (Schwartz et al., 2012) is apparent in heavily
fractured, thin-bedded silt and sandstones of the Permian Hasen Creek Formation that underlie the
valley’s glaciers. Just downstream, the lithology changes to volcaniclastic sediments of the Nikolai
Greenstone Formation (MacKevett, 1979).
THE FLAT CREEK GLACIER DETACHMENTS
On 2013-08-05, the lowermost 500 m of Flat Creek Glacier (below 2270 m asl) detached and traveled 11
km downstream (Fig. 2). The remaining ice responded rapidly, advancing 30–45 m in the days following
the detachment (measured with orthophotos from 2013-08-11 and 2013-09-05) and thinned by up to 28.1
± 0.7 m (Fig. 3). We estimated elevation changes by differencing two digital elevation models (DEMs)
from before and after the detachment (2012-08-26 and 2014-10-12). The total detachment volume was 6.8
± 0.2 x 106 m3 to 11.2 ± 0.7 x 106 m3 (Fig. 3, methods see suppl. data). The lower bound only considers
the elevation difference in the detachment zone. The upper bound further includes the thinning of the
upper glacier as an estimate of the volume that advanced into the detachment zone in response to the
collapse.
Throughout summer 2013 to spring 2015, the remaining glacier advanced and crumbled at the
front, covering the original detachment zone with loose ice. Sometime between 2015-07-18 and 2015-07-
25, this loose ice detached and traveled 10 km down the valley (see suppl. data). On 2015-07-30, another
17.6 ± 0.2 x 106 m3 to 20.1 ± 0.3 x 106 m3 of ice and lithic material detached. This failure reached the
drainage divide at 2650 m asl (Fig. 2 & 3). The resulting mass flow spread debris over 8 km2 of the
alluvial fan, burying 3 km2 of mature forest (at least 4-centuries old; see suppl. data). The angle of the
exposed glacier bed – presumably the failure plane – was 21° above horizontal.
In both 2013 and 2015, the detached masses transformed into highly-mobile mass flows that
reached the White River (12 km downstream) in minutes and ran an average of 76 m up the back of West
Hill, a prominent bedrock knob adjacent to Flat Creek (Fig. 1). Using runup heights (Iverson et al., 2016;
Prochaska, 2008) and the duration of the detachment-induced quakes recorded at the Barnard Glacier
seismic station (60 km SW of Flat Creek), we derived peak velocities up to 50 m/s and mean velocities
around 30 m/s for both events (see suppl. data). Surveying the detachment deposits in 2018 and 2019, we
found fine-grained lithic material (30–40 % clay, see suppl. data) mixed with interstitial ice and rounded
ice blocks. The lithic material was almost exclusively Hasen Creek mudstone from under the glacier.
DETACHMENT DRIVERS
Photographs of the detachment zone acquired with an unmanned aerial vehicle in 2018 show that the thin-
bedded mud and sandstones erode into thick layers of fine-grained, unconsolidated sediment. Despite the
proximity of the Totschunda Fault, we found no seismic triggers for the detachments in the US
Geological Survey (USGS) earthquake record.
One of Flat Creek Glacier’s remarkable features before the first detachment was thick, bulging
ice behind a thin, crevasse-free tongue (Fig. 2). From the length of the shadows cast by the bulge in a
2009-07-13 orthophoto, we constrained the maximum height of the bulge to 70.2 ± 9.4 m (see methods
suppl.). We rule out the possibility that the bulge was caused by a bedrock step because the post-
detachment DEM shows no such feature and it is unlikely that such a feature would have endured
centuries of glacial erosion, yet disintegrate during the detachment (Fig. 3). We found no change in the
horizontal position of the bulge between 2009 and 2011. However, between 2011 and 2013-06-22
(coincident with the surge of the glacier in the adjacent drainage), satellite images show that the bulge
advanced by as much as 100 m (Fig. 2; suppl. data), suggesting that a mass redistribution was underway.
In contrast, the glacier terminus did not advance during this time, supporting our inference of a cold-ice
tongue. The bulge and cold-ice tongue very closely resemble the geometry observed in 1980 on Trapridge
Glacier, 80 km SE (Clarke & Blake, 1991). Englacial temperature measurements on Trapridge Glacier
showed that a thin, cold-ice tongue served as a mechanical dam to temperate ice up-glacier, forming the
bulge. Given the morphological similarities to Trapridge Glacier, a mean annual air temperature of -
12.1°C at the pre-detachment terminus, and continuous permafrost in the headwall, we conclude that Flat
Creek Glacier was polythermal, with a thin cold-ice tongue slowing the advance of thicker, temperate ice
up-glacier.
Based on Flat Creek Glacier’s thermal regime, we infer that subglacial drainage was restricted by
the cold-ice tongue. Glacier marginal-streams and deeply incised supraglacial streams on many of the
region’s small glaciers suggest that this mechanism is common in this area (Irvine-Fynn et al., 2011;
Ryser et al., 2013). Observations from Trapridge suggest that water likely drains through the subglacial
substrate to ice-marginal streams, and we suggest the same was true at Flat Creek Glacier. The limited
efficiency of this drainage mechanism causes water to accumulate if the input rate exceeds the output rate
(Clarke et al., 1984; Clarke & Blake, 1991). To identify where below Flat Creek Glacier water would
have accumulated, we applied a Rho8 flow routing analysis to the 2012-08-26 DEM (Fairfield &
Leymarie, 1991, see methods suppl.). Glacier surface topography is taken as an acceptable catchment-
level proxy for water drainage below the glacier (Igneczi et al., 2018). We find that the area immediately
upstream of the bulge received water from a larger catchment than any other point on the glacier. The
next highest flow concentrations were under the detachment zone. Given this large drainage area and the
crevassed surface of the glacier upstream of the bulge, meltwater likely reached the bed and increased the
subglacial water pressure.
To evaluate the availability of liquid water prior to the detachments, we used a 36-year record of
dynamically-downscaled ERA-Interim temperature and precipitation data available for Alaska at 20 km
resolution (Bieniek et al., 2016; see methods suppl.), bias-corrected with ten years of weather station data
from Chisana. Since both failures happened during peak melt season, we calculated the cumulative
summer water availability for each year by summing rainfall and melt from April through July. Melt was
modeled at an hourly resolution using a degree-day approach with melt factors of 2.7 mm d-1 °C-1 for
snow and 4.87 mm d-1 °C-1 for ice (see methods suppl.; Hock, 2003). At Flat Creek, according to our
model, the cumulative summer water availability preceding the 2013 detachment exceeded the 36-year
mean cumulative summer water availability by 100 – 615 %, or 3.59 – 4.77 standard deviations (𝜎),
depending on elevation (Fig. 4). Water availability was lower than average (-0.49 – 0.03 𝜎) in 2014, but
again exceeded the mean by 0.08 – 0.91 𝜎 in 2015.
DISCUSSION
The apparent emergence of large-scale glacier detachments (Kääb et al., 2018; Falaschi et al., 2018; Paul,
2019; Jacquemart & Loso, 2019) raises the question of whether these events share common drivers, and
whether these will be exacerbated by current warming.
The 2013 detachment at Flat Creek Glacier coincided with unprecedented water availability
driven by record warm temperatures. Our modeled water availability is supported by Alaska-wide
measurements showing 2013 to be the year with the most negative mass balance since 2003 (Wouters,
2019). Due to the inefficient drainage mechanism identified at Flat Creek, the high melt rates allowed
water to accumulate under the glacier, increasing the water pressure in the subglacial till and weak
bedrock. The ultimate shear strength of subglacial till has been shown to increase linearly with effective
normal stress (Iverson et al., 1998). By reducing the effective pressure, increasing basal water pressure is
therefore likely to have weakened the subglacial till. Indeed, the high clay content of the deposits
indicates that the failure initiated within the glacier’s basal substrate. Meanwhile, the advancing bulge
upstream of the cold-ice tongue contributed to increased driving stresses. When meltwater input peaked in
July 2013, rising subglacial water pressures and increased driving stresses allowed the glacier tongue to
detach about 100 m upstream of the 2009 - 2011 location of the bulge.
In 2015, the geometry of the glacier was dramatically altered and we assume that all remaining
ice was temperate. However, the inverse correlation between water availability and glacier stability, and
the role of the weak basal substrate, continued. No detachment occurred in 2014, when water availability
was below average, while activity resumed with increasing water availability in 2015. The precursory
detachment of the loose ice accumulated in the detachment zone shows how easily the underlying lithic
material failed with increased water availability. Under the remaining glacier, the stability of the till may
have been compromised by two factors following the 2013 detachment: (1) reduction of the effective
normal stress due to thinning of the glacier (though this also reduces driving stresses), and (2) alignment
of clay particles by the glacier advance, an effect that has also been shown to reduce the shear strength of
glacial tills (Iverson, 1998). Combined, these factors likely contributed to the 2015 detachment, and also
highlight that a polythermal regime is not a mandatory prerequisite for a large-scale detachment.
Both the 2013 and 2015 mass flows impacted a large swath of 400 year old forest, indicating that
no event of comparable size has occurred here in the past 4 centuries. This suggests that large-scale
glacier detachments may indeed be a new hazard of our warming world.
A comparison with the Kolka and Aru detachments reveal that conditions at Flat Creek strongly
resemble those at Aru, but not those at Kolka. Kolka Glacier is temperate and the stress regime was likely
altered by an accumulation of debris from a series of ice and rock falls (Haeberli et al., 2004, Evans et al.,
2009). In contrast, the cold-ice margins of the Aru glaciers allowed water to accumulate in the subglacial
till over the 5 – 6 years preceding the detachments. Simultaneously, increasing flow velocities were
observed on bulging, temperate ice encroaching upon the tongues of both glaciers, increasing driving
stresses (Gilbert et al., 2018). Under this altered stress regime, the accumulation of water decreased the
effective normal stress on the till, inducing failure in 2016, the year with the highest recorded degree-day
sum (Kääb et al., 2018).
In conclusion, insights from this study suggest that remarkably similar glacial and climatic
conditions led to the Flat Creek and Aru detachments. At Flat Creek Glacier, these conditions led to two
detachments which both produced highly destructive mass flows with wide-reaching impacts, luckily
without human casualties or damage to infrastructure. Our work highlights the potential sensitivity of
soft-bedded polythermal glaciers to sudden detachments under warming conditions, and the need to refine
the criteria that distinguish collapse-prone glaciers from others in this broad category. Identifying which
glaciers are mostly likely to detach is critical to risk management in mountain environments.
Fig. 1: Study area: Glacier and alluvial fan changes (orange & purple box) are shown in detail in Fig. 2.
Yellow dots indicate the locations of electrical resistivity tomography surveys, ground temperatures were
measured at ERT-1. Cyan lines are from the Randolph Glacier Inventory 6.0 (RGI Consortium, 2017).
Flat Creek Glacier is labeled FCG. Note that the background image shows the watershed prior to the
detachments (© Planet, 2018).
Fig. 2: Changes of Flat Creek Glacier and the alluvial fan (orange & purple box in Fig. 1). Panel a) Image
from 2013-08-11. The orange star indicates the accumulation point of water based on the flow
accumulation analysis. Panel b) Image from 2015-08-13. All images © Planet
Panel c) Crevasse-free tongue of Flat Creek Glacier and thicker, crevassed ice upstream. Ikonos image
from 2009-07-13. The shadow used to estimate bulge height is indicated with a white arrow. Yellow and
magenta lines are the edge of the bulge in 2009 and 2013, respectively. © Maxar
Fig. 3: Top left: Surface elevation change between 2012-08-26 (AK IfSAR DEM) and 2014-10-12. Top
right: Surface elevation change between 2014-10-12 and 2016-03-13 (both ArcticDEM, Porter et al.,
2018). The inset maps resolve more detail over the detachments (dashed outlines), the black line is the
original glacier outline. Note the ongoing surge of the glacier west of Flat Creek.
Bottom: Longitudinal profiles from 2012, 2014, and 2016. Below the 2013 detachment line, loose ice
(area shaded green) masked the full surface change.
Fig. 4: Total summer (April - July) water availability at Flat Creek depending on elevation and mean
decadal water availability for an elevation of 2100 m asl.
Acknowledgements
We acknowledge a NASA Earth and Space Science Fellowship for M. Jacquemart and funding from the
NPS Inventory and Monitoring Program. E. Berthier acknowledges funding CNES funding. Field work
Pre-detachment total liquid water availability
1980 1985 1990 1995 2000 2005 2010 2015
Year
0
100
200
300
400
500
Water availability (mm)
Elevation (m asl)
2100
2300
2500
2700
decadal mean
was partially funded under NASA IDS award 80NSSC17K0017, as was K. Tiampo. We thank J. Trop, T.
Vaden, P. Claus, and L. Wassink for early field observations. Valuable input was received from A. Kääb,
M. Dokukin, K. Allstadt, D. Farinotti, A. Vieli, W. Haeberli, and G. Wolken. We thank R. Hooke and A.
Gilbert as well as one anonymous reviewer for their valuable comments.
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