Australia: The Land Where Time Began |
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Thwaites Glacier, West Antarctica Heterogeneous Retreat and Ice Melt
Over the last few decades glaciers that flow into the Amundsen Sea
Embayment in West Antarctica have been increasing in speed and their
grounding line has been retreating. Milillo et
al. have used a constellation
of satellites which have detected the evolution of the velocity of the
ice, thinning of the ice, and retreat of the grounding lines of the
Thwaites Glacier from 1992-2017. A complex pattern of retreat and ice
melt, with sectors that have retreated at 0.8 km/year and floating ice
that has melted at 200 m/year, while others have retreated at 0.3
km/year and ice melting 10 times slower. They interpreted the results in
terms of buoyancy/slope-driven intrusion of seawater along preferred
channels at tidal frequencies that have led to more efficient melting in
cavities that were newly formed. Coupled ice sheet/ocean models do not
yet have such complexities represented.
The Antarctic Ice Sheet is rapidly changing and contributing notably to
global sea level rise (Church et al., 2011; Alley et al., 2015). With a
potential sea level equivalent of 1.2 m. The Amundsen Sea Embayment
(ASE) sector of west Antarctica is presently a dominant contributor to
sea level rise, as well as for decades to come (Joughin, Smith & Medley,
2014; Rignot et al., 2014; DeConto & Pollard, 2016). A third of the mass
loss (Sutterley et al., 2014) from the Amundsen Sea Embayment is
accounted for by the Thwaites Glacier. The main trunk of the Thwaites
Glacier, which is fast flowing, accelerated by 0.8 km/year, or 33%,
between 1973 and 1996, and another 33% between 2006 and 2013 (Mouginot,
Rignot & Scheuchl, 2014). The ice discharge increased by 2.2 Gt/year2,
and the rate quadrupled in 2003-2010 (9.5 Gt/year2). More
recently, some parts of the glacier have been observed to thin by as
much as 4 m/year (McMillan et al., 2014).
Beneath the Thwaites Glacier, as the bed topography is several hundred
metres below sea level at the grounding line and is getting deeper
inland (retrograde bed slope), this sector may be prone to rapid retreat
(Hughes, 1981; Schoof, 2007). It has been suggested by several studies
that the glacier is already in a stage of collapse and the retreat is
not stoppable (Joughin, Smith & Medley, 2014; Rignot et al., 2014;
Parizek et al., 2013). The rate of retreat of the grounding line is
controlled by bed topography, dynamic ice thinning, and melt of the ice
shelf by warm, salty circumpolar deep water (CDW), with a critical role
being played by melting of the ice shelf (Seroussi et al., 2017). The
grounding line retreated by 0.6 to 0.9 km/year between 1996 and 2011,
along the sides of the glacier and the main trunk, respectively (Rignot
et al., 2014). After 2011, there has been no adequate interferometric
synthetic radar (InSAR) data to observe the grounding line retreat (Khazendar
et al., 2016; Scheuchl et al., 2016).
In Fig. 1 of the article the rapid migration of ice was not expected
because the bed is prograde at that location, i.e., the elevation of the
bed rises in the inland direction, which should be conducive to a slower
rate of retreat for a given rate of ice thinning (Alley et al., 2015;
DeConto & Pollard, 2016; Schoof, 2007). At B, the migration is slower,
with a lower rate of shelf thinning, though at that location the slope
of the bed is almost flat or even retrograde, which would be expected to
favour retreat that is more rapid for a given rate of thinning.
According to Milillo et al.
the newly formed cavity at B is thin, which does not favour intrusion of
warm Circumpolar Deep Water from geostrophic flow and efficient vertical
mixing (Joughin et al., 2016;
Jenkins, 2011) and explains the low rates of ice shelf melt. Contrasting
with this the prograde at A favours the opening of a new cavity in the
ice shelf, stronger intrusion of CDW, and efficient mixing with melt
rates that are 20 times higher than those at B. Melting of the ice shelf
at A exceeds the values that were used in numerical ice sheet/ocean
models by factors of 2 to 3 (Joughin, Smith & Medley, 2014; Khazendar et
al., 2016). The melt rate at
B is low versus numerical simulations. Milillo et
al. also found that the
intensity of the melt along the ice at A, that was newly ungrounded, is
correlated linearly with the slope of the ice draft along the direction
that is perpendicular to the gradient in melt, consistent with the plume
theory (Jenkins, 2011). No such correlation exists at B. Geostrophic and
buoyancy/slope-driven flows are inefficient in the thin cavity near B,
which is likely to be dominated by tidal mixing (Holland, 2008).
It is revealed by the TDX data at D that there is formation of a
subglacial channel prior to ungrounding, followed by rapid melting along
the sides near C and E. The D channel is initially 1.2 ± 0.2 km wide.
There is no change in speed along the channel, therefore no dynamic
thinning; melt by the ocean reflects ice thinning (Millgate et
al., 2013). Ice shelf melt is
high along prograde slopes along the sides as for A and low along
retrograde slopes as for B where there less efficient cavity
formation. A process of ice melt via channel intrusion that differs from
the diffusive process that takes place along the grounding zone near A
is revealed by these observations.
The melt rates of the ice shelf that have been discussed were calculated
by use of a Eulerian framework, i.e., at a fixed location in space, in
order to capture melt rates of the ice shelf and ungrounds of the ice
shelf. Milillo et al. also
calculated the melt rates in a Lagrangian framework, where ice blocks
are tracked with time and corrected for flow divergence. The Lagrangian
calculation does not apply on land, on areas that are partially
grounded, or where ice is depressed flow flotation then rebounds during
retreat. Milillo et al.
confirmed ice shelf melt rates of up to 50 m/year on the butterfly and
up to 200 m/year near the main trunk, with large spatial variations,
away from these zones.
The observations of Milillo et al.
contrast with the traditional view on the interaction between ice and
ocean at grounding lines.
1.
Melt channels 1 to 2 km wide and cavities that were newly formed less
than 100 m high would require ocean models to operate at the
subkilometre horizontal scale and sub-100 vertical scale in order to
replicate the melt processes responsible for forming the cavities, which
is a challenge.
2.
As the melt rates in the main trunk are 2 to 3 times higher than those
in models limits the ability of models to reproduce the ice retreat at
those locations.
3.
Ocean-induced ice melt in the main trunk of the Thwaites Glacier occurs
over a 2.5 km wide grounding zone, whereas fixed grounding lines are
used by numerical ice sheet models, i.e., are not affected by tidal
mixing (Joughin, Smith & Medley, 2014; DeConto & Pollard, 2016; Schoof,
2007; Parizek et al., 2013;
Seroussi et al., 2017), with
zero melt applied to the grounding line.
The existence of wide grounding zones, with a distinctive melt regime,
narrow cavities, and nonzero ice melt over the entire grounding zone is
revealed by the results of Milillo et
al. The ice shelf rates may
be lower along retrograde slopes than along prograde slopes, which is
another observation to be explored in detail with ice-ocean models.
Milillo et al. concluded that
the shape of the cavity, including the slope of the bed, bumps, and
hollows in the bed, influences the ocean heat access to the glacier as
well as ocean-induced melt rates.
This study detected the highest rates of retreat at the heads of major
channels of transport of CDW to the main trunk and TEIS (Schmeltz,
Rignot & MacAyeal, 2001), with slow retreat in between (E to F), where
ice is grounded on a ridge. Recent numerical models (Seroussi et
al., 2017) have replicated
the more rapid retreat of TEIS verses the remainder of the glacier and
the mean retreat rate of 0.8 km/year since 1992; therefore it
demonstrates that model skills and boundary conditions have improved
considerably. However, the recent models do not replicate the fast
retreat rate along the main trunk of the Thwaites Glacier, partly
because in that region the ice shelf buttressing is limited. Milillo et
al. report that in that
region heterogeneous melt up to 200 m/year, with large tidal migration
of the grounding line as well as significant melting of ice over the
entire zone of tidal migration. Milillo et
al. suggest that this
configuration calls into question the concept of a fixed grounding line
with zero melt because models that use melt at the grounding line
predict retreat that is more rapid. Therefore, detailed studies of the
grounding zone and its specific regime of ice melt will be critical to
explore in more detail using numerical models, data from remote sensing,
and in situ observations to
improve the characterisation of retreat of the Thwaites Glacier near its
grounding line, its rate of mass loss, and, in turn, its contribution to
global sea level rise in decades to come.
Milillo, P., et al. (2019). "Heterogeneous retreat and ice melt of
Thwaites Glacier, West Antarctica." Science Advances 5(1):
eaau3433. |
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Author: M.H.Monroe Email: admin@austhrutime.com Sources & Further reading |