Feltham, Danny
Arctic sea ice reduction: the evidence, models and impacts Journal Article
In: Philos. Trans. A Math. Phys. Eng. Sci., vol. 373, no. 2045, pp. 20140171, 2015.
BibTeX | Tags:
@article{Feltham2015-sj,
title = {Arctic sea ice reduction: the evidence, models and impacts},
author = {Danny Feltham},
year = {2015},
date = {2015-07-01},
journal = {Philos. Trans. A Math. Phys. Eng. Sci.},
volume = {373},
number = {2045},
pages = {20140171},
publisher = {The Royal Society},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
Serreze, Mark C; Stroeve, Julienne
Arctic sea ice trends, variability and implications for seasonal ice forecasting Journal Article
In: Philos. Trans. A Math. Phys. Eng. Sci., vol. 373, no. 2045, pp. 20140159, 2015.
@article{Serreze2015-pl,
title = {Arctic sea ice trends, variability and implications for seasonal
ice forecasting},
author = {Mark C Serreze and Julienne Stroeve},
year = {2015},
date = {2015-07-01},
journal = {Philos. Trans. A Math. Phys. Eng. Sci.},
volume = {373},
number = {2045},
pages = {20140159},
publisher = {The Royal Society},
abstract = {September Arctic sea ice extent over the period of satellite
observations has a strong downward trend, accompanied by
pronounced interannual variability with a detrended 1 year lag
autocorrelation of essentially zero. We argue that through a
combination of thinning and associated processes related to a
warming climate (a stronger albedo feedback, a longer melt
season, the lack of especially cold winters) the downward trend
itself is steepening. The lack of autocorrelation manifests both
the inherent large variability in summer atmospheric circulation
patterns and that oceanic heat loss in winter acts as a negative
(stabilizing) feedback, albeit insufficient to counter the
steepening trend. These findings have implications for seasonal
ice forecasting. In particular, while advances in observing sea
ice thickness and assimilating thickness into coupled forecast
systems have improved forecast skill, there remains an inherent
limit to predictability owing to the largely chaotic nature of
atmospheric variability.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
observations has a strong downward trend, accompanied by
pronounced interannual variability with a detrended 1 year lag
autocorrelation of essentially zero. We argue that through a
combination of thinning and associated processes related to a
warming climate (a stronger albedo feedback, a longer melt
season, the lack of especially cold winters) the downward trend
itself is steepening. The lack of autocorrelation manifests both
the inherent large variability in summer atmospheric circulation
patterns and that oceanic heat loss in winter acts as a negative
(stabilizing) feedback, albeit insufficient to counter the
steepening trend. These findings have implications for seasonal
ice forecasting. In particular, while advances in observing sea
ice thickness and assimilating thickness into coupled forecast
systems have improved forecast skill, there remains an inherent
limit to predictability owing to the largely chaotic nature of
atmospheric variability.
Boisvert, L N; Stroeve, J C
The Arctic is becoming warmer and wetter as revealed by the Atmospheric Infrared Sounder Journal Article
In: Geophys. Res. Lett., vol. 42, no. 11, pp. 4439–4446, 2015.
@article{Boisvert2015-ry,
title = {The Arctic is becoming warmer and wetter as revealed by the
Atmospheric Infrared Sounder},
author = {L N Boisvert and J C Stroeve},
year = {2015},
date = {2015-06-01},
journal = {Geophys. Res. Lett.},
volume = {42},
number = {11},
pages = {4439–4446},
publisher = {American Geophysical Union (AGU)},
abstract = {AbstractOver the past decade, the Arctic has seen unprecedented
declines in the summer sea ice area, leading to larger and
longer exposed open water areas. The Atmospheric Infrared
Sounder is a useful yet underutilized tool to study
corresponding atmospheric changes and their feedbacks between
2003 and 2013. Most pronounced warming occurs between November
and April, with skin and air temperatures increasing on average
2.5 K and 1.5 K over the Arctic Ocean. In response to sea ice
loss, evaporation rates (i.e., moisture flux) increased between
August and October by 1.5 $times$ 10−3 g m−2 s−1 (3.8 W m−2
latent heat flux energy), increasing the water vapor feedback
and cloud cover. Although most trends are positive over the
Arctic Ocean, there is considerable interannual variability.
Increasing specific humidity in May and corresponding downward
moisture fluxes cause earlier melt onset; warming skin
temperatures and radiative responses to increased water vapor
and cloud cover in autumn delay freeze‐up.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
declines in the summer sea ice area, leading to larger and
longer exposed open water areas. The Atmospheric Infrared
Sounder is a useful yet underutilized tool to study
corresponding atmospheric changes and their feedbacks between
2003 and 2013. Most pronounced warming occurs between November
and April, with skin and air temperatures increasing on average
2.5 K and 1.5 K over the Arctic Ocean. In response to sea ice
loss, evaporation rates (i.e., moisture flux) increased between
August and October by 1.5 $times$ 10−3 g m−2 s−1 (3.8 W m−2
latent heat flux energy), increasing the water vapor feedback
and cloud cover. Although most trends are positive over the
Arctic Ocean, there is considerable interannual variability.
Increasing specific humidity in May and corresponding downward
moisture fluxes cause earlier melt onset; warming skin
temperatures and radiative responses to increased water vapor
and cloud cover in autumn delay freeze‐up.
Paul, Frank; Bolch, Tobias; Kääb, Andreas; Nagler, Thomas; Nuth, Christopher; Scharrer, Killian; Shepherd, Andrew; Strozzi, Tazio; Ticconi, Francesca; Bhambri, Rakesh; Berthier, Etienne; Bevan, Suzanne; Gourmelen, Noel; Heid, Torborg; Jeong, Seongsu; Kunz, Matthias; Lauknes, Tom Rune; Luckman, Adrian; Boncori, John Peter Merryman; Moholdt, Geir; Muir, Alan; Neelmeijer, Julia; Rankl, Melanie; VanLooy, Jeffrey; Niel, Thomas Van
The glaciers climate change initiative: Methods for creating glacier area, elevation change and velocity products Journal Article
In: Remote Sens. Environ., vol. 162, pp. 408–426, 2015.
@article{Paul2015-nc,
title = {The glaciers climate change initiative: Methods for creating
glacier area, elevation change and velocity products},
author = {Frank Paul and Tobias Bolch and Andreas Kääb and Thomas Nagler and Christopher Nuth and Killian Scharrer and Andrew Shepherd and Tazio Strozzi and Francesca Ticconi and Rakesh Bhambri and Etienne Berthier and Suzanne Bevan and Noel Gourmelen and Torborg Heid and Seongsu Jeong and Matthias Kunz and Tom Rune Lauknes and Adrian Luckman and John Peter Merryman Boncori and Geir Moholdt and Alan Muir and Julia Neelmeijer and Melanie Rankl and Jeffrey VanLooy and Thomas Van Niel},
year = {2015},
date = {2015-06-01},
journal = {Remote Sens. Environ.},
volume = {162},
pages = {408–426},
publisher = {Elsevier BV},
abstract = {Glaciers and their changes through time are increasingly
obtained from a wide range of satellite sensors. Due to the
often remote location of glaciers in inaccessible and
high-mountain terrain, satellite observations frequently provide
the only available measurements. Furthermore, satellite data
provide observations of glacier characteristics that are
difficult to monitor using ground-based measurements, thus
complementing the latter. In the Glaciers_cci project of the
European Space Agency (ESA), three of these characteristics are
investigated in detail: glacier area, elevation change and
surface velocity. We use (a) data from optical sensors to derive
glacier outlines, (b) digital elevation models from at least two
points in time, (c) repeat altimetry for determining elevation
changes, and (d) data from repeat optical and microwave sensors
for calculating surface velocity. For the latter, the two sensor
types provide complementary information in terms of
spatio-temporal coverage. While (c) and (d) can be generated
mostly automatically, (a) and (b) require the intervention of an
analyst. Largely based on the results of various round robin
experiments (multi-analyst benchmark studies) for each of the
products, we suggest and describe the most suitable algorithms
for product creation and provide recommendations concerning
their practical implementation and the required post-processing.
For some of the products (area, velocity) post-processing can
influence product quality more than the main-processing
algorithm.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
obtained from a wide range of satellite sensors. Due to the
often remote location of glaciers in inaccessible and
high-mountain terrain, satellite observations frequently provide
the only available measurements. Furthermore, satellite data
provide observations of glacier characteristics that are
difficult to monitor using ground-based measurements, thus
complementing the latter. In the Glaciers_cci project of the
European Space Agency (ESA), three of these characteristics are
investigated in detail: glacier area, elevation change and
surface velocity. We use (a) data from optical sensors to derive
glacier outlines, (b) digital elevation models from at least two
points in time, (c) repeat altimetry for determining elevation
changes, and (d) data from repeat optical and microwave sensors
for calculating surface velocity. For the latter, the two sensor
types provide complementary information in terms of
spatio-temporal coverage. While (c) and (d) can be generated
mostly automatically, (a) and (b) require the intervention of an
analyst. Largely based on the results of various round robin
experiments (multi-analyst benchmark studies) for each of the
products, we suggest and describe the most suitable algorithms
for product creation and provide recommendations concerning
their practical implementation and the required post-processing.
For some of the products (area, velocity) post-processing can
influence product quality more than the main-processing
algorithm.
Gomez, N; Gregoire, L J; Mitrovica, J X; Payne, A J
Laurentide‐Cordilleran Ice Sheet saddle collapse as a contribution to meltwater pulse 1A Journal Article
In: Geophys. Res. Lett., vol. 42, no. 10, pp. 3954–3962, 2015.
@article{Gomez2015-lm,
title = {Laurentide‐Cordilleran Ice Sheet saddle collapse as a
contribution to meltwater pulse 1A},
author = {N Gomez and L J Gregoire and J X Mitrovica and A J Payne},
year = {2015},
date = {2015-05-01},
journal = {Geophys. Res. Lett.},
volume = {42},
number = {10},
pages = {3954–3962},
publisher = {American Geophysical Union (AGU)},
abstract = {AbstractThe source or sources of meltwater pulse 1A (MWP‐1A) at
~14.5 ka, recorded at widely distributed sites as a sea level
rise of ~10–20 m in less than 500 years, is uncertain. A recent
ice modeling study of North America and Greenland has suggested
that the collapse of an ice saddle between the Laurentide and
Cordilleran ice sheets, with a eustatic sea level equivalent
(ESLE) of ~10 m, may have been the dominant contributor to
MWP‐1A. To test this suggestion, we predict gravitationally
self‐consistent sea level changes from the Last Glacial Maximum
to the present day associated with the ice model. We find that a
combination of the saddle collapse scenario and melting outside
North America and Greenland with an ESLE of ~3 m yields sea
level changes across MWP‐1A that are consistent with far‐field
sea level records at Barbados, Tahiti, and Sunda Shelf.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
~14.5 ka, recorded at widely distributed sites as a sea level
rise of ~10–20 m in less than 500 years, is uncertain. A recent
ice modeling study of North America and Greenland has suggested
that the collapse of an ice saddle between the Laurentide and
Cordilleran ice sheets, with a eustatic sea level equivalent
(ESLE) of ~10 m, may have been the dominant contributor to
MWP‐1A. To test this suggestion, we predict gravitationally
self‐consistent sea level changes from the Last Glacial Maximum
to the present day associated with the ice model. We find that a
combination of the saddle collapse scenario and melting outside
North America and Greenland with an ESLE of ~3 m yields sea
level changes across MWP‐1A that are consistent with far‐field
sea level records at Barbados, Tahiti, and Sunda Shelf.
Lecomte, Olivier; Fichefet, Thierry; Flocco, Daniela; Schroeder, David; Vancoppenolle, Martin
Interactions between wind-blown snow redistribution and melt ponds in a coupled ocean–sea ice model Journal Article
In: Ocean Model. (Oxf.), vol. 87, pp. 67–80, 2015.
@article{Lecomte2015-xc,
title = {Interactions between wind-blown snow redistribution and melt
ponds in a coupled ocean–sea ice model},
author = {Olivier Lecomte and Thierry Fichefet and Daniela Flocco and David Schroeder and Martin Vancoppenolle},
year = {2015},
date = {2015-03-01},
journal = {Ocean Model. (Oxf.)},
volume = {87},
pages = {67–80},
publisher = {Elsevier BV},
abstract = {Introducing a parameterization of the interactions between
wind-driven snow depth changes and melt pond evolution allows us
to improve large scale models. In this paper we have implemented
an explicit melt pond scheme and, for the first time, a wind
dependant snow redistribution model and new snow thermophysics
into a coupled ocean–sea ice model.The comparison of long-term
mean statistics of melt pond fractions against observations
demonstrates realistic melt pond cover on average over Arctic
sea ice, but a clear underestimation of the pond coverage on the
multi-year ice (MYI) of the western Arctic Ocean. The latter
shortcoming originates from the concealing effect of persistent
snow on forming ponds, impeding their growth. Analyzing a second
simulation with intensified snow drift enables the
identification of two distinct modes of sensitivity in the melt
pond formation process. First, the larger proportion of
wind-transported snow that is lost in leads directly curtails
the late spring snow volume on sea ice and facilitates the early
development of melt ponds on MYI. In contrast, a combination of
higher air temperatures and thinner snow prior to the onset of
melting sometimes make the snow cover switch to a regime where
it melts entirely and rapidly. In the latter situation,
seemingly more frequent on first-year ice (FYI), a smaller snow
volume directly relates to a reduced melt pond
cover.Notwithstanding, changes in snow and water accumulation on
seasonal sea ice is naturally limited, which lessens the impacts
of wind-blown snow redistribution on FYI, as compared to those
on MYI. At the basin scale, the overall increased melt pond
cover results in decreased ice volume via the ice-albedo
feedback in summer, which is experienced almost exclusively by
MYI.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
wind-driven snow depth changes and melt pond evolution allows us
to improve large scale models. In this paper we have implemented
an explicit melt pond scheme and, for the first time, a wind
dependant snow redistribution model and new snow thermophysics
into a coupled ocean–sea ice model.The comparison of long-term
mean statistics of melt pond fractions against observations
demonstrates realistic melt pond cover on average over Arctic
sea ice, but a clear underestimation of the pond coverage on the
multi-year ice (MYI) of the western Arctic Ocean. The latter
shortcoming originates from the concealing effect of persistent
snow on forming ponds, impeding their growth. Analyzing a second
simulation with intensified snow drift enables the
identification of two distinct modes of sensitivity in the melt
pond formation process. First, the larger proportion of
wind-transported snow that is lost in leads directly curtails
the late spring snow volume on sea ice and facilitates the early
development of melt ponds on MYI. In contrast, a combination of
higher air temperatures and thinner snow prior to the onset of
melting sometimes make the snow cover switch to a regime where
it melts entirely and rapidly. In the latter situation,
seemingly more frequent on first-year ice (FYI), a smaller snow
volume directly relates to a reduced melt pond
cover.Notwithstanding, changes in snow and water accumulation on
seasonal sea ice is naturally limited, which lessens the impacts
of wind-blown snow redistribution on FYI, as compared to those
on MYI. At the basin scale, the overall increased melt pond
cover results in decreased ice volume via the ice-albedo
feedback in summer, which is experienced almost exclusively by
MYI.
Lecomte, Olivier; Fichefet, Thierry; Flocco, Daniela; Schroeder, David; Vancoppenolle, Martin
Interactions between wind-blown snow redistribution and melt ponds in a coupled ocean–sea ice model Journal Article
In: Ocean Model. (Oxf.), vol. 87, pp. 67–80, 2015.
@article{Lecomte2015-xj,
title = {Interactions between wind-blown snow redistribution and melt
ponds in a coupled ocean–sea ice model},
author = {Olivier Lecomte and Thierry Fichefet and Daniela Flocco and David Schroeder and Martin Vancoppenolle},
year = {2015},
date = {2015-03-01},
journal = {Ocean Model. (Oxf.)},
volume = {87},
pages = {67–80},
publisher = {Elsevier BV},
abstract = {Introducing a parameterization of the interactions between
wind-driven snow depth changes and melt pond evolution allows us
to improve large scale models. In this paper we have implemented
an explicit melt pond scheme and, for the first time, a wind
dependant snow redistribution model and new snow thermophysics
into a coupled ocean–sea ice model.The comparison of long-term
mean statistics of melt pond fractions against observations
demonstrates realistic melt pond cover on average over Arctic
sea ice, but a clear underestimation of the pond coverage on the
multi-year ice (MYI) of the western Arctic Ocean. The latter
shortcoming originates from the concealing effect of persistent
snow on forming ponds, impeding their growth. Analyzing a second
simulation with intensified snow drift enables the
identification of two distinct modes of sensitivity in the melt
pond formation process. First, the larger proportion of
wind-transported snow that is lost in leads directly curtails
the late spring snow volume on sea ice and facilitates the early
development of melt ponds on MYI. In contrast, a combination of
higher air temperatures and thinner snow prior to the onset of
melting sometimes make the snow cover switch to a regime where
it melts entirely and rapidly. In the latter situation,
seemingly more frequent on first-year ice (FYI), a smaller snow
volume directly relates to a reduced melt pond
cover.Notwithstanding, changes in snow and water accumulation on
seasonal sea ice is naturally limited, which lessens the impacts
of wind-blown snow redistribution on FYI, as compared to those
on MYI. At the basin scale, the overall increased melt pond
cover results in decreased ice volume via the ice-albedo
feedback in summer, which is experienced almost exclusively by
MYI.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
wind-driven snow depth changes and melt pond evolution allows us
to improve large scale models. In this paper we have implemented
an explicit melt pond scheme and, for the first time, a wind
dependant snow redistribution model and new snow thermophysics
into a coupled ocean–sea ice model.The comparison of long-term
mean statistics of melt pond fractions against observations
demonstrates realistic melt pond cover on average over Arctic
sea ice, but a clear underestimation of the pond coverage on the
multi-year ice (MYI) of the western Arctic Ocean. The latter
shortcoming originates from the concealing effect of persistent
snow on forming ponds, impeding their growth. Analyzing a second
simulation with intensified snow drift enables the
identification of two distinct modes of sensitivity in the melt
pond formation process. First, the larger proportion of
wind-transported snow that is lost in leads directly curtails
the late spring snow volume on sea ice and facilitates the early
development of melt ponds on MYI. In contrast, a combination of
higher air temperatures and thinner snow prior to the onset of
melting sometimes make the snow cover switch to a regime where
it melts entirely and rapidly. In the latter situation,
seemingly more frequent on first-year ice (FYI), a smaller snow
volume directly relates to a reduced melt pond
cover.Notwithstanding, changes in snow and water accumulation on
seasonal sea ice is naturally limited, which lessens the impacts
of wind-blown snow redistribution on FYI, as compared to those
on MYI. At the basin scale, the overall increased melt pond
cover results in decreased ice volume via the ice-albedo
feedback in summer, which is experienced almost exclusively by
MYI.
Flocco, Daniela; Feltham, Daniel L; Bailey, Eleanor; Schroeder, David
The refreezing of melt ponds on Arctic sea ice Journal Article
In: J. Geophys. Res. Oceans, vol. 120, no. 2, pp. 647–659, 2015.
@article{Flocco2015-wo,
title = {The refreezing of melt ponds on Arctic sea ice},
author = {Daniela Flocco and Daniel L Feltham and Eleanor Bailey and David Schroeder},
year = {2015},
date = {2015-02-01},
journal = {J. Geophys. Res. Oceans},
volume = {120},
number = {2},
pages = {647–659},
publisher = {American Geophysical Union (AGU)},
abstract = {AbstractThe presence of melt ponds on the surface of Arctic sea
ice significantly reduces its albedo, inducing a positive
feedback leading to sea ice thinning. While the role of melt
ponds in enhancing the summer melt of sea ice is well known,
their impact on suppressing winter freezing of sea ice has,
hitherto, received less attention. Melt ponds freeze by forming
an ice lid at the upper surface, which insulates them from the
atmosphere and traps pond water between the underlying sea ice
and the ice lid. The pond water is a store of latent heat, which
is released during refreezing. Until a pond freezes completely,
there can be minimal ice growth at the base of the underlying
sea ice. In this work, we present a model of the refreezing of a
melt pond that includes the heat and salt balances in the ice
lid, trapped pond, and underlying sea ice. The model uses a
two‐stream radiation model to account for radiative scattering
at phase boundaries. Simulations and related sensitivity studies
suggest that trapped pond water may survive for over a month. We
focus on the role that pond salinity has on delaying the
refreezing process and retarding basal sea ice growth. We
estimate that for a typical sea ice pond coverage in autumn,
excluding the impact of trapped ponds in models overestimates
ice growth by up to 265 million km3, an overestimate of 26%.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
ice significantly reduces its albedo, inducing a positive
feedback leading to sea ice thinning. While the role of melt
ponds in enhancing the summer melt of sea ice is well known,
their impact on suppressing winter freezing of sea ice has,
hitherto, received less attention. Melt ponds freeze by forming
an ice lid at the upper surface, which insulates them from the
atmosphere and traps pond water between the underlying sea ice
and the ice lid. The pond water is a store of latent heat, which
is released during refreezing. Until a pond freezes completely,
there can be minimal ice growth at the base of the underlying
sea ice. In this work, we present a model of the refreezing of a
melt pond that includes the heat and salt balances in the ice
lid, trapped pond, and underlying sea ice. The model uses a
two‐stream radiation model to account for radiative scattering
at phase boundaries. Simulations and related sensitivity studies
suggest that trapped pond water may survive for over a month. We
focus on the role that pond salinity has on delaying the
refreezing process and retarding basal sea ice growth. We
estimate that for a typical sea ice pond coverage in autumn,
excluding the impact of trapped ponds in models overestimates
ice growth by up to 265 million km3, an overestimate of 26%.
Bulczak, Anna I; Bacon, Sheldon; Garabato, Alberto C Naveira; Ridout, Andrew; Sonnewald, Maike J P; Laxon, Seymour W
Seasonal variability of sea surface height in the coastal waters and deep basins of the Nordic Seas Journal Article
In: Geophys. Res. Lett., vol. 42, no. 1, pp. 113–120, 2015.
BibTeX | Tags:
@article{Bulczak2015-ia,
title = {Seasonal variability of sea surface height in the coastal waters
and deep basins of the Nordic Seas},
author = {Anna I Bulczak and Sheldon Bacon and Alberto C Naveira Garabato and Andrew Ridout and Maike J P Sonnewald and Seymour W Laxon},
year = {2015},
date = {2015-01-01},
journal = {Geophys. Res. Lett.},
volume = {42},
number = {1},
pages = {113–120},
publisher = {American Geophysical Union (AGU)},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
Leeson, A A; Shepherd, A; Briggs, K; Howat, I; Fettweis, X; Morlighem, M; Rignot, E
Supraglacial lakes on the Greenland ice sheet advance inland under warming climate Journal Article
In: Nat. Clim. Chang., vol. 5, no. 1, pp. 51–55, 2015.
@article{Leeson2015-ek,
title = {Supraglacial lakes on the Greenland ice sheet advance inland
under warming climate},
author = {A A Leeson and A Shepherd and K Briggs and I Howat and X Fettweis and M Morlighem and E Rignot},
year = {2015},
date = {2015-01-01},
journal = {Nat. Clim. Chang.},
volume = {5},
number = {1},
pages = {51–55},
publisher = {Springer Science and Business Media LLC},
abstract = {Supraglacial lakes (SGLs) form annually on the Greenland ice
sheet and, when they drain, their discharge enhances ice-sheet
flow by lubricating the base and potentially by warming the ice.
Today, SGLs tend to form within the ablation zone, where
enhanced lubrication is offset by efficient subglacial drainage.
However, it is not clear what impact a warming climate will have
on this arrangement. Here, we use an SGL initiation and growth
model to show that lakes form at higher altitudes as
temperatures rise, consistent with satellite observations. Our
simulations show that in southwest Greenland, SGLs spread 103
and 110 km further inland by the year 2060 under moderate (RCP
4.5) and extreme (RCP 8.5) climate change scenarios,
respectively, leading to an estimated 48-53% increase in the
area over which they are distributed across the ice sheet as a
whole. Up to half of these new lakes may be large enough to
drain, potentially delivering water and heat to the ice-sheet
base in regions where subglacial drainage is inefficient. In
such places, ice flow responds positively to increases in
surface water delivered to the bed through enhanced basal
lubrication and warming of the ice, and so the inland advance of
SGLs should be considered in projections of ice-sheet change.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
sheet and, when they drain, their discharge enhances ice-sheet
flow by lubricating the base and potentially by warming the ice.
Today, SGLs tend to form within the ablation zone, where
enhanced lubrication is offset by efficient subglacial drainage.
However, it is not clear what impact a warming climate will have
on this arrangement. Here, we use an SGL initiation and growth
model to show that lakes form at higher altitudes as
temperatures rise, consistent with satellite observations. Our
simulations show that in southwest Greenland, SGLs spread 103
and 110 km further inland by the year 2060 under moderate (RCP
4.5) and extreme (RCP 8.5) climate change scenarios,
respectively, leading to an estimated 48-53% increase in the
area over which they are distributed across the ice sheet as a
whole. Up to half of these new lakes may be large enough to
drain, potentially delivering water and heat to the ice-sheet
base in regions where subglacial drainage is inefficient. In
such places, ice flow responds positively to increases in
surface water delivered to the bed through enhanced basal
lubrication and warming of the ice, and so the inland advance of
SGLs should be considered in projections of ice-sheet change.
Levinsen, J F; Khvorostovsky, K; Ticconi, F; Shepherd, A; Forsberg, R; Sørensen, L S; Muir, A; Pie, N; Felikson, D; Flament, T; Hurkmans, R; Moholdt, G; Gunter, B; Lindenbergh, R C; Kleinherenbrink, M
ESA ice sheet CCI: derivation of the optimal method for surface elevation change detection of the Greenland ice sheet – round robin results Journal Article
In: Int. J. Remote Sens., vol. 36, no. 2, pp. 551–573, 2015.
@article{Levinsen2015-lc,
title = {ESA ice sheet CCI: derivation of the optimal method for
surface elevation change detection of the Greenland ice sheet –
round robin results},
author = {J F Levinsen and K Khvorostovsky and F Ticconi and A Shepherd and R Forsberg and L S Sørensen and A Muir and N Pie and D Felikson and T Flament and R Hurkmans and G Moholdt and B Gunter and R C Lindenbergh and M Kleinherenbrink},
year = {2015},
date = {2015-01-01},
journal = {Int. J. Remote Sens.},
volume = {36},
number = {2},
pages = {551–573},
publisher = {Informa UK Limited},
abstract = {For more than two decades, radar altimetry missions have
provided continuous elevation estimates of the Greenland ice
sheet (GrIS). Here, we propose a method for using such data to
estimate ice-sheet-wide surface elevation changes (SECs). The
final data set will be based on observations acquired from the
European Space Agency's Environmental Satellite (ENVISAT),
European Remote Sensing (ERS)-1 and -2, CryoSat-2, and, in the
longer term, Sentinel-3 satellites. In order to find the
best-performing method, an intercomparison exercise has been
carried out in which the scientific community was asked to
provide their best SEC estimates as well as feedback sheets
describing the applied method. Due to the hitherto few
radar-based SEC analyses as well as the higher accuracy of laser
data, the participants were asked to use either ENVISAT radar or
ICESat (Ice, Cloud, and land Elevation Satellite) laser
altimetry over the Jakobshavn Isbræ drainage basin. The
submissions were validated against airborne laser-scanner data,
and intercomparisons were carried out to analyse the potential
of the applied methods and to find whether the two altimeters
were capable of resolving the same signal. The analyses found
great potential of the applied repeat-track and cross-over
techniques, and, for the first time over Greenland, that
repeat-track analyses from radar altimetry agreed well with
laser data. Since topography-related errors can be neglected in
cross-over analyses, it is expected that the most accurate,
ice-sheet-wide SEC estimates are obtained by combining the
cross-over and repeat-track techniques. It is thus possible to
exploit the high accuracy of the former and the large spatial
data coverage of the latter. Based on CryoSat's different
operation modes, and the increased spatial and temporal data
coverage, this shows good potential for a future inclusion of
CryoSat-2 and Sentinel-3 data to continuously obtain accurate
SEC estimates both in the interior and margin ice sheet.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
provided continuous elevation estimates of the Greenland ice
sheet (GrIS). Here, we propose a method for using such data to
estimate ice-sheet-wide surface elevation changes (SECs). The
final data set will be based on observations acquired from the
European Space Agency's Environmental Satellite (ENVISAT),
European Remote Sensing (ERS)-1 and -2, CryoSat-2, and, in the
longer term, Sentinel-3 satellites. In order to find the
best-performing method, an intercomparison exercise has been
carried out in which the scientific community was asked to
provide their best SEC estimates as well as feedback sheets
describing the applied method. Due to the hitherto few
radar-based SEC analyses as well as the higher accuracy of laser
data, the participants were asked to use either ENVISAT radar or
ICESat (Ice, Cloud, and land Elevation Satellite) laser
altimetry over the Jakobshavn Isbræ drainage basin. The
submissions were validated against airborne laser-scanner data,
and intercomparisons were carried out to analyse the potential
of the applied methods and to find whether the two altimeters
were capable of resolving the same signal. The analyses found
great potential of the applied repeat-track and cross-over
techniques, and, for the first time over Greenland, that
repeat-track analyses from radar altimetry agreed well with
laser data. Since topography-related errors can be neglected in
cross-over analyses, it is expected that the most accurate,
ice-sheet-wide SEC estimates are obtained by combining the
cross-over and repeat-track techniques. It is thus possible to
exploit the high accuracy of the former and the large spatial
data coverage of the latter. Based on CryoSat's different
operation modes, and the increased spatial and temporal data
coverage, this shows good potential for a future inclusion of
CryoSat-2 and Sentinel-3 data to continuously obtain accurate
SEC estimates both in the interior and margin ice sheet.
Morris, Elizabeth M; Wingham, Duncan J
Uncertainty in mass-balance trends derived from altimetry: a case study along the EGIG line, central Greenland Journal Article
In: J. Glaciol., vol. 61, no. 226, pp. 345–356, 2015.
@article{Morris2015-dz,
title = {Uncertainty in mass-balance trends derived from altimetry: a
case study along the EGIG line, central Greenland},
author = {Elizabeth M Morris and Duncan J Wingham},
year = {2015},
date = {2015-01-01},
journal = {J. Glaciol.},
volume = {61},
number = {226},
pages = {345–356},
publisher = {Cambridge University Press (CUP)},
abstract = {AbstractRepeated measurements of density profiles and surface
elevation along a 515 km traverse of the Greenland ice sheet are
used to determine elevation change rates and the error in
determining mass-balance trends from these rates which arises
from short-term fluctuations in mass input, compaction and
surface density. Mean values of this error, averaged over 100 km
sections of the traverse, decrease with time from the start of
observations in 2004, with a half-time of ∼4 years. After 7
years the mean error is less than the ice equivalent mass
imbalance.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
elevation along a 515 km traverse of the Greenland ice sheet are
used to determine elevation change rates and the error in
determining mass-balance trends from these rates which arises
from short-term fluctuations in mass input, compaction and
surface density. Mean values of this error, averaged over 100 km
sections of the traverse, decrease with time from the start of
observations in 2004, with a half-time of ∼4 years. After 7
years the mean error is less than the ice equivalent mass
imbalance.
McMillan, Malcolm; Shepherd, Andrew; Gourmelen, Noel; Dehecq, Amaury; Leeson, Amber; Ridout, Andrew; Flament, Thomas; Hogg, Anna; Gilbert, Lin; Benham, Toby; Broeke, Michiel; Dowdeswell, Julian A; Fettweis, Xavier; Noël, Brice; Strozzi, Tazio
Rapid dynamic activation of a marine‐based Arctic ice cap Journal Article
In: Geophys. Res. Lett., vol. 41, no. 24, pp. 8902–8909, 2014.
@article{McMillan2014-yj,
title = {Rapid dynamic activation of a marine‐based Arctic ice cap},
author = {Malcolm McMillan and Andrew Shepherd and Noel Gourmelen and Amaury Dehecq and Amber Leeson and Andrew Ridout and Thomas Flament and Anna Hogg and Lin Gilbert and Toby Benham and Michiel Broeke and Julian A Dowdeswell and Xavier Fettweis and Brice Noël and Tazio Strozzi},
year = {2014},
date = {2014-12-01},
journal = {Geophys. Res. Lett.},
volume = {41},
number = {24},
pages = {8902–8909},
publisher = {American Geophysical Union (AGU)},
abstract = {AbstractWe use satellite observations to document rapid
acceleration and ice loss from a formerly slow‐flowing,
marine‐based sector of Austfonna, the largest ice cap in the
Eurasian Arctic. During the past two decades, the sector ice
discharge has increased 45‐fold, the velocity regime has
switched from predominantly slow (~ 101 m/yr) to fast (~ 103
m/yr) flow, and rates of ice thinning have exceeded 25 m/yr. At
the time of widespread dynamic activation, parts of the terminus
may have been near floatation. Subsequently, the imbalance has
propagated 50 km inland to within 8 km of the ice cap summit.
Our observations demonstrate the ability of slow‐flowing ice to
mobilize and quickly transmit the dynamic imbalance inland; a
process that we show has initiated rapid ice loss to the ocean
and redistribution of ice mass to locations more susceptible to
melt, yet which remains poorly understood.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
acceleration and ice loss from a formerly slow‐flowing,
marine‐based sector of Austfonna, the largest ice cap in the
Eurasian Arctic. During the past two decades, the sector ice
discharge has increased 45‐fold, the velocity regime has
switched from predominantly slow (~ 101 m/yr) to fast (~ 103
m/yr) flow, and rates of ice thinning have exceeded 25 m/yr. At
the time of widespread dynamic activation, parts of the terminus
may have been near floatation. Subsequently, the imbalance has
propagated 50 km inland to within 8 km of the ice cap summit.
Our observations demonstrate the ability of slow‐flowing ice to
mobilize and quickly transmit the dynamic imbalance inland; a
process that we show has initiated rapid ice loss to the ocean
and redistribution of ice mass to locations more susceptible to
melt, yet which remains poorly understood.
Roberts, William H G; Valdes, Paul J; Payne, Antony J
Topography's crucial role in Heinrich Events Journal Article
In: Proc. Natl. Acad. Sci. U. S. A., vol. 111, no. 47, pp. 16688–16693, 2014.
Abstract | BibTeX | Tags: North Atlantic; abrupt climate changes; ice sheet−climate interactions
@article{Roberts2014-ra,
title = {Topography's crucial role in Heinrich Events},
author = {William H G Roberts and Paul J Valdes and Antony J Payne},
year = {2014},
date = {2014-11-01},
journal = {Proc. Natl. Acad. Sci. U. S. A.},
volume = {111},
number = {47},
pages = {16688–16693},
publisher = {Proceedings of the National Academy of Sciences},
abstract = {Heinrich Events, the abrupt changes in the Laurentide Ice Sheet
that cause the appearance of the well-observed Heinrich Layers,
are thought to have a strong effect on the global climate. The
focus of most studies that have looked at the climate's response
to these events has been the freshwater flux that results from
melting icebergs. However, there is the possibility that the
varying height of the ice sheet could force a change in the
climate. In this study, we present results from a newly
developed coupled climate/ice sheet model to show what effect
this topographic change has both on its own and in concert with
the flux of freshwater from melting icebergs. We show that the
topographic forcing can explain a number of the climate changes
that are observed during Heinrich Events, such as the warming
and wettening in Florida and the warm sea surface temperatures
in the central North Atlantic, which freshwater forcing alone
cannot. We also find regions, for example the tropical Atlantic,
where the response is a mixture of the two: Here observations
may help disentangle the relative importance of each mechanism.
These results suggest that the simple paradigm of a Heinrich
Event causing climate change via freshwater inputs into the
North Atlantic needs to be revised.},
keywords = {North Atlantic; abrupt climate changes; ice sheet−climate interactions},
pubstate = {published},
tppubtype = {article}
}
that cause the appearance of the well-observed Heinrich Layers,
are thought to have a strong effect on the global climate. The
focus of most studies that have looked at the climate's response
to these events has been the freshwater flux that results from
melting icebergs. However, there is the possibility that the
varying height of the ice sheet could force a change in the
climate. In this study, we present results from a newly
developed coupled climate/ice sheet model to show what effect
this topographic change has both on its own and in concert with
the flux of freshwater from melting icebergs. We show that the
topographic forcing can explain a number of the climate changes
that are observed during Heinrich Events, such as the warming
and wettening in Florida and the warm sea surface temperatures
in the central North Atlantic, which freshwater forcing alone
cannot. We also find regions, for example the tropical Atlantic,
where the response is a mixture of the two: Here observations
may help disentangle the relative importance of each mechanism.
These results suggest that the simple paradigm of a Heinrich
Event causing climate change via freshwater inputs into the
North Atlantic needs to be revised.
Wright, A P; Brocq, A M Le; Cornford, S L; Bingham, R G; Corr, H F J; Ferraccioli, F; Jordan, T A; Payne, A J; Rippin, D M; Ross, N; Siegert, M J
Sensitivity of the Weddell Sea sector ice streams to sub-shelf melting and surface accumulation Journal Article
In: Cryosphere, vol. 8, no. 6, pp. 2119–2134, 2014.
@article{Wright2014-nj,
title = {Sensitivity of the Weddell Sea sector ice streams to sub-shelf
melting and surface accumulation},
author = {A P Wright and A M Le Brocq and S L Cornford and R G Bingham and H F J Corr and F Ferraccioli and T A Jordan and A J Payne and D M Rippin and N Ross and M J Siegert},
year = {2014},
date = {2014-11-01},
journal = {Cryosphere},
volume = {8},
number = {6},
pages = {2119–2134},
publisher = {Copernicus GmbH},
abstract = {Abstract. A recent ocean modelling study indicates that possible
changes in circulation may bring warm deep-ocean water into
direct contact with the grounding lines of the Filchner–Ronne
ice streams, suggesting the potential for future ice losses from
this sector equivalent to ~0.3 m of sea-level rise. Significant
advancements have been made in our knowledge of both the basal
topography and ice velocity in the Weddell Sea sector, and the
ability to accurately model marine ice sheet dynamics, thus
enabling an assessment to be made of the relative sensitivities
of the diverse collection of ice streams feeding the
Filchner–Ronne Ice Shelf. Here we use the BISICLES ice sheet
model, which employs adaptive-mesh refinement to resolve
grounding line dynamics, to carry out such an assessment. The
impact of realistic perturbations to the surface and sub-shelf
mass balance forcing fields from our 2000-year ``reference''
model run indicate that both the Institute and Möller ice
streams are highly sensitive to changes in basal melting either
near to their respective grounding lines, or in the region of
the ice rises within the Filchner–Ronne Ice Shelf. These same
perturbations have little impact, however, on the Rutford,
Carlson or Foundation ice streams, while the Evans Ice Stream is
found to enter a phase of unstable retreat only after melt at
its grounding line has increased by 50% of likely present-day
values.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
changes in circulation may bring warm deep-ocean water into
direct contact with the grounding lines of the Filchner–Ronne
ice streams, suggesting the potential for future ice losses from
this sector equivalent to ~0.3 m of sea-level rise. Significant
advancements have been made in our knowledge of both the basal
topography and ice velocity in the Weddell Sea sector, and the
ability to accurately model marine ice sheet dynamics, thus
enabling an assessment to be made of the relative sensitivities
of the diverse collection of ice streams feeding the
Filchner–Ronne Ice Shelf. Here we use the BISICLES ice sheet
model, which employs adaptive-mesh refinement to resolve
grounding line dynamics, to carry out such an assessment. The
impact of realistic perturbations to the surface and sub-shelf
mass balance forcing fields from our 2000-year ``reference''
model run indicate that both the Institute and Möller ice
streams are highly sensitive to changes in basal melting either
near to their respective grounding lines, or in the region of
the ice rises within the Filchner–Ronne Ice Shelf. These same
perturbations have little impact, however, on the Rutford,
Carlson or Foundation ice streams, while the Evans Ice Stream is
found to enter a phase of unstable retreat only after melt at
its grounding line has increased by 50% of likely present-day
values.
Heorton, Harold D B S; Feltham, Daniel L; Hunt, Julian C R
The response of the sea ice edge to atmospheric and oceanic jet formation Journal Article
In: J. Phys. Oceanogr., vol. 44, no. 9, pp. 2292–2316, 2014.
@article{Heorton2014-gy,
title = {The response of the sea ice edge to atmospheric and oceanic jet
formation},
author = {Harold D B S Heorton and Daniel L Feltham and Julian C R Hunt},
year = {2014},
date = {2014-09-01},
journal = {J. Phys. Oceanogr.},
volume = {44},
number = {9},
pages = {2292–2316},
publisher = {American Meteorological Society},
abstract = {AbstractThe sea ice edge presents a region of many feedback
processes between the atmosphere, ocean, and sea ice (Maslowski
et al.). Here the authors focus on the impact of on-ice
atmospheric and oceanic flows at the sea ice edge. Mesoscale jet
formation due to the Coriolis effect is well understood over
sharp changes in surface roughness such as coastlines (Hunt et
al.). This sharp change in surface roughness is experienced by
the atmosphere and ocean encountering a compacted sea ice edge.
This paper presents a study of a dynamic sea ice edge responding
to prescribed atmospheric and oceanic jet formation. An
idealized analytical model of sea ice drift is developed and
compared to a sea ice climate model [the Los Alamos Sea Ice
Model (CICE)] run on an idealized domain. The response of the
CICE model to jet formation is tested at various resolutions.It
is found that the formation of atmospheric jets at the sea ice
edge increases the wind speed parallel to the sea ice edge and
results in the formation of a sea ice drift jet in agreement
with an observed sea ice drift jet (Johannessen et al.). The
increase in ice drift speed is dependent upon the angle between
the ice edge and wind and results in up to a 40% increase in
ice transport along the sea ice edge. The possibility of oceanic
jet formation and the resultant effect upon the sea ice edge is
less conclusive. Observations and climate model data of the
polar oceans have been analyzed to show areas of likely
atmospheric jet formation, with the Fram Strait being of
particular interest.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
processes between the atmosphere, ocean, and sea ice (Maslowski
et al.). Here the authors focus on the impact of on-ice
atmospheric and oceanic flows at the sea ice edge. Mesoscale jet
formation due to the Coriolis effect is well understood over
sharp changes in surface roughness such as coastlines (Hunt et
al.). This sharp change in surface roughness is experienced by
the atmosphere and ocean encountering a compacted sea ice edge.
This paper presents a study of a dynamic sea ice edge responding
to prescribed atmospheric and oceanic jet formation. An
idealized analytical model of sea ice drift is developed and
compared to a sea ice climate model [the Los Alamos Sea Ice
Model (CICE)] run on an idealized domain. The response of the
CICE model to jet formation is tested at various resolutions.It
is found that the formation of atmospheric jets at the sea ice
edge increases the wind speed parallel to the sea ice edge and
results in the formation of a sea ice drift jet in agreement
with an observed sea ice drift jet (Johannessen et al.). The
increase in ice drift speed is dependent upon the angle between
the ice edge and wind and results in up to a 40% increase in
ice transport along the sea ice edge. The possibility of oceanic
jet formation and the resultant effect upon the sea ice edge is
less conclusive. Observations and climate model data of the
polar oceans have been analyzed to show areas of likely
atmospheric jet formation, with the Fram Strait being of
particular interest.
Jenouvrier, Stéphanie; Holland, Marika; Stroeve, Julienne; Serreze, Mark; Barbraud, Christophe; Weimerskirch, Henri; Caswell, Hal
Projected continent-wide declines of the emperor penguin under climate change Journal Article
In: Nat. Clim. Chang., vol. 4, no. 8, pp. 715–718, 2014.
@article{Jenouvrier2014-vd,
title = {Projected continent-wide declines of the emperor penguin under
climate change},
author = {Stéphanie Jenouvrier and Marika Holland and Julienne Stroeve and Mark Serreze and Christophe Barbraud and Henri Weimerskirch and Hal Caswell},
year = {2014},
date = {2014-08-01},
journal = {Nat. Clim. Chang.},
volume = {4},
number = {8},
pages = {715–718},
publisher = {Springer Science and Business Media LLC},
abstract = {Climate change has been projected to affect species
distribution1 and future trends of local populations2, 3, but
projections of global population trends are rare. We analyse
global population trends of the emperor penguin (Aptenodytes
forsteri), an iconic Antarctic top predator, under the influence
of sea ice conditions projected by coupled climate models
assessed in the Intergovernmental Panel on Climate Change (IPCC)
effort4. We project the dynamics of all 45 known emperor penguin
colonies5 by forcing a sea-ice-dependent demographic model6, 7
with local, colony-specific, sea ice conditions projected
through to the end of the twenty-first century. Dynamics differ
among colonies, but by 2100 all populations are projected to be
declining. At least two-thirds are projected to have declined by
>50% from their current size. The global population is
projected to have declined by at least 19%. Because criteria to
classify species by their extinction risk are based on the
global population dynamics8, global analyses are critical for
conservation9. We discuss uncertainties arising in such global
projections and the problems of defining conservation criteria
for species endangered by future climate change.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
distribution1 and future trends of local populations2, 3, but
projections of global population trends are rare. We analyse
global population trends of the emperor penguin (Aptenodytes
forsteri), an iconic Antarctic top predator, under the influence
of sea ice conditions projected by coupled climate models
assessed in the Intergovernmental Panel on Climate Change (IPCC)
effort4. We project the dynamics of all 45 known emperor penguin
colonies5 by forcing a sea-ice-dependent demographic model6, 7
with local, colony-specific, sea ice conditions projected
through to the end of the twenty-first century. Dynamics differ
among colonies, but by 2100 all populations are projected to be
declining. At least two-thirds are projected to have declined by
>50% from their current size. The global population is
projected to have declined by at least 19%. Because criteria to
classify species by their extinction risk are based on the
global population dynamics8, global analyses are critical for
conservation9. We discuss uncertainties arising in such global
projections and the problems of defining conservation criteria
for species endangered by future climate change.
Levermann, A; Winkelmann, R; Nowicki, S; Fastook, J L; Frieler, K; Greve, R; Hellmer, H H; Martin, M A; Meinshausen, M; Mengel, M; Payne, A J; Pollard, D; Sato, T; Timmermann, R; Wang, W L; Bindschadler, R A
Projecting Antarctic ice discharge using response functions from SeaRISE ice-sheet models Journal Article
In: Earth Syst. Dyn., vol. 5, no. 2, pp. 271–293, 2014.
@article{Levermann2014-tk,
title = {Projecting Antarctic ice discharge using response functions from
SeaRISE ice-sheet models},
author = {A Levermann and R Winkelmann and S Nowicki and J L Fastook and K Frieler and R Greve and H H Hellmer and M A Martin and M Meinshausen and M Mengel and A J Payne and D Pollard and T Sato and R Timmermann and W L Wang and R A Bindschadler},
year = {2014},
date = {2014-08-01},
journal = {Earth Syst. Dyn.},
volume = {5},
number = {2},
pages = {271–293},
publisher = {Copernicus GmbH},
abstract = {Abstract. The largest uncertainty in projections of future
sea-level change results from the potentially changing dynamical
ice discharge from Antarctica. Basal ice-shelf melting induced
by a warming ocean has been identified as a major cause for
additional ice flow across the grounding line. Here we attempt
to estimate the uncertainty range of future ice discharge from
Antarctica by combining uncertainty in the climatic forcing, the
oceanic response and the ice-sheet model response. The
uncertainty in the global mean temperature increase is obtained
from historically constrained emulations with the MAGICC-6.0
(Model for the Assessment of Greenhouse gas Induced Climate
Change) model. The oceanic forcing is derived from scaling of
the subsurface with the atmospheric warming from 19
comprehensive climate models of the Coupled Model
Intercomparison Project (CMIP-5) and two ocean models from the
EU-project Ice2Sea. The dynamic ice-sheet response is derived
from linear response functions for basal ice-shelf melting for
four different Antarctic drainage regions using experiments from
the Sea-level Response to Ice Sheet Evolution (SeaRISE)
intercomparison project with five different Antarctic ice-sheet
models. The resulting uncertainty range for the historic
Antarctic contribution to global sea-level rise from 1992 to
2011 agrees with the observed contribution for this period if we
use the three ice-sheet models with an explicit representation
of ice-shelf dynamics and account for the time-delayed warming
of the oceanic subsurface compared to the surface air
temperature. The median of the additional ice loss for the 21st
century is computed to 0.07 m (66% range: 0.02–0.14 m; 90%
range: 0.0–0.23 m) of global sea-level equivalent for the
low-emission RCP-2.6 (Representative Concentration Pathway)
scenario and 0.09 m (66% range: 0.04–0.21 m; 90% range:
0.01–0.37 m) for the strongest RCP-8.5. Assuming no time delay
between the atmospheric warming and the oceanic subsurface,
these values increase to 0.09 m (66% range: 0.04–0.17 m; 90%
range: 0.02–0.25 m) for RCP-2.6 and 0.15 m (66% range:
0.07–0.28 m; 90% range: 0.04–0.43 m) for RCP-8.5. All
probability distributions are highly skewed towards high values.
The applied ice-sheet models are coarse resolution with
limitations in the representation of grounding-line motion.
Within the constraints of the applied methods, the uncertainty
induced from different ice-sheet models is smaller than that
induced by the external forcing to the ice sheets.},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
sea-level change results from the potentially changing dynamical
ice discharge from Antarctica. Basal ice-shelf melting induced
by a warming ocean has been identified as a major cause for
additional ice flow across the grounding line. Here we attempt
to estimate the uncertainty range of future ice discharge from
Antarctica by combining uncertainty in the climatic forcing, the
oceanic response and the ice-sheet model response. The
uncertainty in the global mean temperature increase is obtained
from historically constrained emulations with the MAGICC-6.0
(Model for the Assessment of Greenhouse gas Induced Climate
Change) model. The oceanic forcing is derived from scaling of
the subsurface with the atmospheric warming from 19
comprehensive climate models of the Coupled Model
Intercomparison Project (CMIP-5) and two ocean models from the
EU-project Ice2Sea. The dynamic ice-sheet response is derived
from linear response functions for basal ice-shelf melting for
four different Antarctic drainage regions using experiments from
the Sea-level Response to Ice Sheet Evolution (SeaRISE)
intercomparison project with five different Antarctic ice-sheet
models. The resulting uncertainty range for the historic
Antarctic contribution to global sea-level rise from 1992 to
2011 agrees with the observed contribution for this period if we
use the three ice-sheet models with an explicit representation
of ice-shelf dynamics and account for the time-delayed warming
of the oceanic subsurface compared to the surface air
temperature. The median of the additional ice loss for the 21st
century is computed to 0.07 m (66% range: 0.02–0.14 m; 90%
range: 0.0–0.23 m) of global sea-level equivalent for the
low-emission RCP-2.6 (Representative Concentration Pathway)
scenario and 0.09 m (66% range: 0.04–0.21 m; 90% range:
0.01–0.37 m) for the strongest RCP-8.5. Assuming no time delay
between the atmospheric warming and the oceanic subsurface,
these values increase to 0.09 m (66% range: 0.04–0.17 m; 90%
range: 0.02–0.25 m) for RCP-2.6 and 0.15 m (66% range:
0.07–0.28 m; 90% range: 0.04–0.43 m) for RCP-8.5. All
probability distributions are highly skewed towards high values.
The applied ice-sheet models are coarse resolution with
limitations in the representation of grounding-line motion.
Within the constraints of the applied methods, the uncertainty
induced from different ice-sheet models is smaller than that
induced by the external forcing to the ice sheets.
Armitage, Thomas W K; Wingham, Duncan J; Ridout, Andy L
Meteorological origin of the static crossover pattern present in low-resolution-mode CryoSat-2 data over central Antarctica Journal Article
In: IEEE Geosci. Remote Sens. Lett., vol. 11, no. 7, pp. 1295–1299, 2014.
BibTeX | Tags:
@article{Armitage2014-vr,
title = {Meteorological origin of the static crossover pattern present in
low-resolution-mode CryoSat-2 data over central Antarctica},
author = {Thomas W K Armitage and Duncan J Wingham and Andy L Ridout},
year = {2014},
date = {2014-07-01},
journal = {IEEE Geosci. Remote Sens. Lett.},
volume = {11},
number = {7},
pages = {1295–1299},
publisher = {Institute of Electrical and Electronics Engineers (IEEE)},
keywords = {},
pubstate = {published},
tppubtype = {article}
}
McMillan, Malcolm; Shepherd, Andrew; Sundal, Aud; Briggs, Kate; Muir, Alan; Ridout, Andrew; Hogg, Anna; Wingham, Duncan
Increased ice losses from Antarctica detected by CryoSat-2 Journal Article
In: Geophys. Res. Lett., vol. 41, no. 11, pp. 3899–3905, 2014.
BibTeX | Tags:
@article{McMillan2014-mc,
title = {Increased ice losses from Antarctica detected by CryoSat-2},
author = {Malcolm McMillan and Andrew Shepherd and Aud Sundal and Kate Briggs and Alan Muir and Andrew Ridout and Anna Hogg and Duncan Wingham},
year = {2014},
date = {2014-06-01},
journal = {Geophys. Res. Lett.},
volume = {41},
number = {11},
pages = {3899–3905},
publisher = {American Geophysical Union (AGU)},
keywords = {},
pubstate = {published},
tppubtype = {article}
}