Drifting snow climate of the Greenland ice sheet: a study with a regional climate model
The Cryosphere, 6, 891–899, 2012
www.the-cryosphere.net/6/891/2012/
doi:10.5194/tc-6-891-2012
© Author(s) 2012. CC Attribution 3.0 License.
The Cryosphere
Drifting snow climate of the Greenland ice sheet:
a study with a regional climate model
J. T. M. Lenaerts1 , M. R. van den Broeke1 , J. H. van Angelen1 , E. van Meijgaard2 , and S. J. Déry3
1 Institute
for Marine and Atmospheric research Utrecht, Utrecht University, Utrecht, The Netherlands
Netherlands Meteorological Institute, De Bilt, The Netherlands
3 University of Northern British Columbia, Prince George, Canada
2 Royal
Correspondence to: J. T. M. Lenaerts ()
Received: 20 March 2012 – Published in The Cryosphere Discuss.: 3 May 2012
Revised: 18 July 2012 – Accepted: 3 August 2012 – Published: 15 August 2012
Abstract. This paper presents the drifting snow climate of
the Greenland ice sheet, using output from a high-resolution
(∼ 11 km) regional climate model. Because reliable direct
observations of drifting snow do not exist, we evaluate
the modeled near-surface climate instead, using automatic
weather station (AWS) observations from the K-transect and
find that RACMO2 realistically simulates near-surface wind
speed and relative humidity, two variables that are important for drifting snow. Integrated over the ice sheet, drifting
snow sublimation (SUds ) equals 24±3 Gt yr−1 , and is significantly larger than surface sublimation (SUs , 16 ± 2 Gt yr−1 ).
SUds strongly varies between seasons, and is only important
in winter, when surface sublimation and runoff are small.
A rapid transition exists between the winter season, when
snowfall and SUds are important, and the summer season,
when snowmelt is significant, which increases surface snow
density and thereby limits drifting snow processes. Drifting
snow erosion (ERds ) is only important on a regional scale.
In recent decades, following decreasing wind speed and rising near-surface temperatures, SUds exhibits a negative trend
(0.1 ± 0.1 Gt yr−1 ), which is compensated by an increase in
SUs of similar magnitude.
1
Introduction
The Greenland ice sheet (GrIS) is the largest body of ice in
the Northern Hemisphere, containing approximately 7 m sea
level equivalent (IPCC AR4). In the last two decades, numerous Greenland outlet glaciers have accelerated and surface mass balance (SMB) has declined (Rignot et al., 2011),
both contributing about equally to recent Greenland mass
loss (Van den Broeke et al., 2009). The volume loss of outlet glaciers may be primarily related to oceanic warming
(Holland et al., 2008), but the interaction between ocean and
outlet glaciers is complex (Nick et al., 2009; Straneo et al.,
2011). At the same time, Greenland has experienced significant atmospheric warming in the recent two decades (Box
and Cohen, 2006), increasing surface meltwater production
and subsequent runoff (Ettema et al., 2009), extending the
length of the melt season (Fettweis et al., 2011) and triggering the melt-albedo feedback (Tedesco et al., 2010).
To assess the surface mass balance (SMB) of the GrIS, regional climate models are useful tools. In the SMB of the
GrIS, precipitation (P ) is the main source of mass, whereas
mass is lost by surface (SUs ) and drifting snow sublimation
(SUds ), drifting snow erosion (ERds ) and meltwater runoff
(RU). ERds is defined as the horizontal divergence of the
snow transport (TRds ). Until now, drifting snow processes
have usually been neglected in GrIS SMB studies (Fettweis,
2007; Hanna et al., 2005; Ettema et al., 2009). On the Antarctic ice sheet, drifting snow sublimation (SUds ) is an important
ablation term in dry and windy areas and ERds redistributes
snow on a local to regional scale (Lenaerts and van den
Broeke, 2012). Several studies estimated SUds for Greenland
(Déry and Yau, 2002; Box et al., 2006) and ERds (Déry and
Yau, 2002), using parameterizations based on wind speed
(Déry and Yau, 1999), neglecting feedbacks to the overlying atmosphere and the snow surface, which are known to
be important (Bintanja, 2001; Lenaerts et al., 2010, 2012a;
Gallée et al., 2001).
Published by Copernicus Publications on behalf of the European Geosciences Union.
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J. T. M. Lenaerts et al.: Greenland drifting snow climate
J. T. M. Lenaerts et al.: Greenland drifting snow climate
Here we present the drifting snow climate (1960–2011)
of the Greenland ice sheet using a regional atmospheric climate model (RACMO2) at relatively high horizontal resolution (11 km). RACMO2 includes an interactive drifting snow
routine (Lenaerts et al., 2012a). We discuss the spatial and
temporal variability of SUds and ERds and their impact on
the SMB of the GrIS.
2
2.1
Methods
Numerical setup
The Regional Atmospheric Climate MOdel version 2
(RACMO2 hereafter; Van Meijgaard et al., 2008) combines the dynamical parameterizations from the HIgh Resolution Limited Area Model (HIRLAM) (Undén et al., 2002)
with the physical schemes from the European Centre for
Medium-Range Weather Forecasts model (ECMWF cycle
23r4, White, 2001). In recent years, RACMO2 has been
used to estimate the SMB of Antarctica (Van de Berg et al.,
2005; Lenaerts et al., 2012b) and Greenland (Ettema et al.,
2009). Modeled precipitation and surface mass balance have
been extensively evaluated using available in-situ observations (Ettema et al., 2009). Moreover, Ettema et al. (2010b)
showed that RACMO2 provides a realistic simulation of the
near-surface climate of the GrIS, although several deficiencies were detected, especially in the snow albedo scheme.
To resolve this, we included a snow albedo parameterization based on the growth of snow during dry and wet metamorphosis, so that snow albedo can be physically coupled
to snow grain size (Flanner and Zender, 2006). This significantly improved net shortwave radiation in RACMO2 over
the Antarctic ice sheet (Kuipers Munneke et al., 2011) and
the length of the melt season in Greenland (Van Angelen
et al., 2012). In addition, a remote sensing-derived background albedo (from the Moderate Resolution Imaging Spectroradiometer, MODIS) is prescribed for ice (Van Angelen
et al., 2012) to capture the spatial variability of albedo in
the ablation area when the winter snow has melted (Van
den Broeke et al., 2008). Finally, the drifting snow scheme
derived from Déry and Yau (1999) has been included in
RACMO2. It calculates drifting snow transport and sublimation, and accounts for interactions between the drifting
snow layer with both the overlying atmosphere and the underlying snow surface (Lenaerts et al., 2010). Furthermore,
we use an empirically derived parameterization for surface
snow density. This was derived by Lenaerts et al. (2012a) for
Antarctica, such that modeled drifting snow frequency and
horizontal transport agree well with available in-situ and remote sensing observations (Lenaerts et al., 2012a).
For the GrIS, RACMO2 has 40 levels in the vertical
and the model grid has a horizontal spacing of ∼ 11 km.
It is forced at its lateral bo (...truncated)