11:30 am |
Cosmopolitan and Provincial Sea Ice in a Transitioning Arctic OceanCosmopolitan and Provincial Sea Ice in a Transitioning Arctic Ocean
Robert Newton, Lamont-Doherty Earth Observatory, bnewton [at] ldeo.columbia.edu
Stephanie Pfirman, Barnard College, spfirman [at] barnard.edu
Bruno Tremblay, McGill University, bruno.tremblay [at] mcgill.ca
Patricia Derepentigny, McGill University, patricia.derepentigny [at] mail.mcgill.ca
We apply a Lagrangian sea ice tracking software to the problem of transport between the exclusive economic zones (EEZs) of the coastal Arctic nations over about 3 decades: 1979-2011. Lagrangian tracking is combined with sea ice concentration maps to distinguish sea ice formation and melt events from ice drift. We describe trends in formation and melt locations and sea-ice transport pathways. Most ice, ca. 60%, melts within 100 km of where it is formed; only ca. 15% escapes from its "native" EEZ. Of the ice that does leave its region of formation, the majority is ultimately exported from the Arctic through Fram Strait, melting in the East Greenland Current. While only a small fraction of sea ice is exported from one nation’s exclusive economic zone to another’s, this transport nonetheless amounts to tens of thousands of square kilometers of sea ice. Over the last three decades, as the ice has thinned, ice travelling between nations has accelerated by about 18% per decade. As a result, the transit times between different shelf seas of the Arctic have declined significantly. The total area of sea ice transported between EEZs has increased, with the rate of increase varying regionally. The rapid thinning (approximately 50% over the satellite era) of ice, however, means that the volume of freshwater transport between EEZs in solid form has probably nonetheless declined. As the summer melt expands, melt competes with transport and even fast-moving ice can be “caught” by the melt front before it can “escape” from its EEZ. We apply our tracking method to climate model output to consider this and other trends will evolve as the Arctic transitions to a seasonally ice-free state.
Robert Newton
Lamont-Doherty Earth Observatory
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11:50 am |
Connections Between the Spring Pacific-Arctic Dipole and Summer Sea Ice in the Beaufort-Chukchi SeasConnections Between the Spring Pacific-Arctic Dipole and Summer Sea Ice in the Beaufort-Chukchi Seas
Minghong Zhang, Bedford Institute of Oceanography, Minghong.zhang [at] dfo-mpo.gc.ca
William perrie, Bedford Institute of Oceanography, William.Perrie [at] dfo-mpo.gc.ca
Zhenxia Long, Bedford Institute of Oceanography, zhenxia.long [at] dfo-mpo.gc.ca
We identified an atmospheric circulation dipole anomaly in the Pacific-Arctic sector and we showed that it is related to the following September sea ice in the Beaufort-Chukchi Sea, using sea ice observations and model-generated data from PIOMAS (Pan-Arctic Ice-Ocean Modeling and Assimilation System), and the European Centre for Medium-Range Weather Forecasts (ECMWF) Re-Analysis. The dipole anomaly is the second leading EOF mode of spring (April-June) sea level pressure (SLP) in the Pacific-Arctic (600N-900N, 1200E-1200W) and it accounts for 21% of the variance. This dipole anomaly, which we denote as the Pacific-Arctic Dipole, has a positive anomaly in the Beaufort Sea and a negative anomaly extending from East Siberia to Northwest America, and it exhibits co-variance with the Beaufort High and the Aleutian Low. The dipole mode also reflects the re-distribution of cyclone activities in the Pacific-Arctic sector, with fewer cyclones in the Beaufort Sea and central Arctic and more cyclones in the subpolar Pacific. We also define a cyclone activity dipole index using the difference between the cyclone system density in the Arctic (700N-900N, 900E-600W) and that in the subpolar Pacific (500N-600N, 1500E-2100W), which is highly correlated with the time series of the Pacific-Arctic Dipole. We found that the spring Pacific-Arctic Dipole accounts for about 20% of the interannual variance of the following summer SIC in the Beaufort-Chukchi Sea. A positive Pacific-Arctic Dipole has an enhanced Beaufort high and the resulting intensified eastern winds in the Beaufort Sea lead to enhanced ice advection and weakened sea ice thickness. Ice is advected into warm Alaskan coastal waters which results in extensive melting. Moreover, less cyclone activity leads to less middle level cloud cover and less warm air advection in the Beaufort Sea and central Arctic, which causes a net surface heat flux gain, resulting in further reductions in sea ice.
Minghong Zhang
Bedford Institute of Oceanography
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12:10 pm |
Impact of Aerosols on Arctic Sea Ice Extent PredictionImpact of Aerosols on Arctic Sea Ice Extent Prediction
Marie-Éve Gagné, Canadian Centre for Climate Modelling and Analysis, Environment Canada , Marie-Eve.Gagne [at] canada.ca
This study considers the influence of both stratospheric and tropospheric aerosol changes on Arctic sea ice extent on interannual to decadal timescales. While it is well-known that accounting for volcanic aerosol increases the skill of interannual to decadal predictions of surface temperature, its impact on sea ice prediction has not been widely considered. Here we analyze the impact of historical volcanoes on Arctic sea ice extent using a large ensemble of 20th-century climate simulations, and demonstrate that an increase in Arctic sea ice extent following these eruptions persists for up to a decade. Even though we do not find a detectable response in observations, these results suggest that inclusion of the effect in seasonal to interannual predictions of sea ice extent should improve skill on these timescales. Secondly, while the influence of future greenhouse gas changes on sea ice extent is known to be important for predictions on decadal timescales, the influence of projected tropospheric aerosol changes has received less attention. We examine the simulated response of Arctic sea ice to projected aerosol and aerosol precursor emissions changes under the Representative Concentration Pathway (RCP) scenarios, and show that projected aerosol emissions decreases drive approximately 20-30% of the projected decrease in annual mean Arctic sea ice extent on decadal timescales.
Marie-Éve Gagné
Canadian Centre for Climate Modelling and Analysis, Environment Canada
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12:30 pm |
Lunch (provided) |
1:40 pm |
Sea Ice Wall of the AntarcticSea Ice Wall of the Antarctic
Douglas Martinson, Lamont-Doherty Earth Observatory, Columbia University, dgm [at] ldeo.columbia.edu
The Antarctic Circumpolar Current Separates the cold polar oceans (density dominated by salinity) from the warm subtropical waters (density controlled by temperature). In the polar oceans cooling of the surface waters in autumn has little effect on the density of the mixed layer, allowing a rather thin surface layer to freeze to the freezing point before sea ice formation. Moving across the ACC, the cooling has a stronger affect on the density and causes convective deepening, eventually deepening the surface to depths that are so deep there is not enough winter sea-air heat loss to cool such a thick layer to the freezing point. There is a location where sea ice simply cannot grow because of this surface layer thickening—that location forming the virtual sea ice wall (SIW). This presentation discusses the underlying physics and shows the location of the SIW. Its climatological position aligns remarkably well with the climatological ice edge suggesting that the wall may actually be restricting the northern extent of the sea ice edge. Discussing the wall is preceded by a presentation of the Antarctic ocean-sea ice interaction, as well as a discussion comparing and contrasting such processes in the Arctic (mainly contrasting).
Keynote Presentation by Douglas Martinson
Lamont-Doherty Earth Observatory, Columbia University
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2:10 pm |
Water Mass Transformation Under Southern Ocean Sea IceWater Mass Transformation Under Southern Ocean Sea Ice
Ryan Abernathey, Lamont–Doherty Earth Observatory, Columbia University, abernethygillisr [at] inac-ainc.gc.ca
This study quantifies the role of Antarctic sea ice in the transformations of water masses within the Southern Ocean State Estimate (SOSE). Winds drive a strong export of sea ice away from the continent towards the open ocean. The resulting freshwater fluxes at the ocean surface dominate the Southern Ocean freshwater budget (compared with direct precipitation and glacial melt), and these strong fluxes have a major impact on density, stratification, and circulation. Using Walin’s water mass transformation framework, we isolate the contributions of brine rejection, ice melt, and snow interception on the modification of seawater density. Together with direct atmospheric precipitation - evaporation, glacial melt, surface heat flux, and interior mixing, these processes provide the thermodynamic transformations necessary to sustain the meridional overturning circulation. The transformation analysis reveals that sea-ice freshwater fluxes are the main contributor to the transformation of upwelling Upper Circumpolar Deep Water, pushing it primarily towards lighter Antarctic Intermediate and Subantarctic Mode Water but also partly toward denser classes. We also examine the seasonal cycle in transformation, revealing a subtle interplay between brine rejection and upper ocean mixing. Overall these results indicate a tight coupling between Antarctic sea ice and the upper branch of the Southern Ocean overturning circulation.
Ryan Abernathey
Lamont–Doherty Earth Observatory, Columbia University
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2:30 pm |
Arctic-Midlatitudes Climate Linkage by Stratosphere-Troposphere Coupling and its Implications in Sea Ice PredictionArctic-Midlatitudes Climate Linkage by Stratosphere-Troposphere Coupling and its Implications in Sea Ice Prediction
Jinro Ukita, Niigata University, jukita [at] env.sc.niigata-u.ac.jp
Hiroyasu Hasumi, University of Tokyo, hasumi [at] aori.u-tokyo.ac.jp
In this talk I will provide a quick overview on Arctic-midlatitdues climate linkage especially by way of stratosphere-troposphere coupling. Evidence is emerging from both observations and model results that under present climate conditions Arctic sea-ice loss results in modulated propagation of planetary-scale Rossby waves, leading to changes in the strength of polar vortex with consequent surface signals. Having gained some knowledge on this process we are beginning to put various components together for sub-seasonal to sub-decadal prediction, for which sea ice serves as both forcing and an output. In the second part, I will discuss about how this implies in sea ice prediction, in particular in the areas of turbulent heat flux and sea-ice regional variability.
Jinro Ukita
Niigata University
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2:50 pm |
Understanding Physical Processes and Evaluating Parameterizations During the 2015 Freeze-Up Season Using a Coupled Sea Ice-Ocean-Atmosphere Forecast Model Understanding Physical Processes and Evaluating Parameterizations During the 2015 Freeze-Up Season Using a Coupled Sea Ice-Ocean-Atmosphere Forecast Model
Amy Solomon, CIRES/University of Colorado and PSD/ESRL/NOAA, amy.solomon [at] noaa.gov
Janet Intrieri, PSD/ESRL/NOAA, Janet.Intrieri [at] noaa.gov
Ola Persson, CIRES/University of Colorado and PSD/ESRL/NOAA, Ola.Persson [at] noaa.gov
Mimi Hughes, CIRES/University of Colorado and PSD/ESRL/NOAA, Mimi.Hughes [at] noaa.gov
Christopher Cox, CIRES/University of Colorado and PSD/ESRL/NOAA, christopher.j.cox [at] noaa.gov
Improved sea ice forecasting must be based on improved model representation of coupled system processes that impact the sea ice thermodynamic and dynamic state. Pertinent coupled system processes remain uncertain and include surface energy fluxes, clouds, precipitation, boundary layer structure, momentum transfer and sea-ice dynamics, interactions between large-scale circulation and local processes, and others.
We will present results, comparisons, process-oriented diagnostics, and parameterization assessment from sea ice forecasts using a version of the Regional Arctic System Model (RASM) adapted for short-term Arctic sea ice forecasting. Specifically, cloud, atmosphere, and ocean observations for studies of atmospheric predictability, air-ocean turbulent fluxes, and sea ice conditions collected in the marginal ice zone from ship-based campaign and coastal Arctic land stations will be used. We will also outline future model improvements based on a comparison of observations that include replacing the mixed-layer ocean model with a multi-layer upper ocean model to allow for observed mixed layer variability, such as storing heat below the surface layer that is transferred up in large storms and horizontal ocean advection.
RASM is a limited-area, fully coupled ice-ocean-atmosphere-land model. It includes the Weather Research and Forecasting (WRF) atmospheric model, the LANL Parallel Ocean Program (POP) and Community Ice Model Version 5 (CICE5) and the NCAR Community Land Model (CLMv4.5) configured for the pan-Arctic region. These components are coupled using a regionalized version of the CESM flux coupler (CPL7), which includes modifications important for resolving the sea ice pack’s inertial response to transient (i.e. weather) events.
In order to optimize the model for short-term forecasts the dynamic level ocean model has been replaced with a mixed–layer ocean model, the horizontal domain is limited to the Arctic, and all components are run with 10km horizontal resolution. This model is run with a bulk double-moment cloud microphysics scheme for droplets and frozen hydrometeors that allows both size and number of hydrometeors to vary in response to environmental conditions (Morrison et al. 2009).
Daily 5-day forecasts with RASM-ESRL were run for the 2015 freeze-up season, initialized with GFS atmosphere and AMSR2 sea ice analyses and forced by 3-hourly GFS forecasts at the lateral boundaries. The forecasts were delivered daily and used for guidance on the UNOLS research vessel Sikuliaq during the SeaState campaign. These daily forecasts have been validated with observations of surface fluxes and vertical profiles of cloud ice and liquid at land sites, and with observations of surface fluxes and sea ice characteristics from recent ship campaign and ice mass balance buoys. These relatively short forecasts are currently being used to validate and improve simulations of synoptic evolution, atmospheric boundary-layer structure and surface energy fluxes over sea ice and the adjacent ocean.
Amy Solomon
Cooperative Institute for Research in Environmental Sciences, University of Colorado and Physical Sciences Division, Earth System Research Laboratory, NOAA
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3:10 pm |
Arctic Sea Ice Thickness from the Cryosat-2 Satellite – Methods, Uncertainties, and Near Real Time Data DeliveryArctic Sea Ice Thickness from the Cryosat-2 Satellite – Methods, Uncertainties, and Near Real Time Data Delivery
Rachel Tilling, University College London, rachel.tilling.12 [at] ucl.ac.uk
Andy Ridout, University College London, a.ridout [at] ucl.ac.uk
Variations in Arctic sea ice thickness and volume affect regional heat and freshwater budgets and patterns of atmospheric circulation at lower latitudes. Estimates of Arctic sea ice thickness and volume can be obtained from observation and model outputs, but so far, an in-depth comparison of these outputs has not occurred. Such a comparison is crucial for the validation of models that form the basis of future Arctic and global climate projections. In order for an in-depth comparison to be successful, expert knowledge is required of numerous model configurations, as well as the observation methods used to estimate sea ice thickness. This presentation will aim to encourage collaboration between modellers and observers by summarising the method used to calculate sea ice thickness from CryoSat-2 radar altimeter satellite observations, and the difficulties and limitations associated with obtaining these.
It is also our hope that the availability of Arctic-wide sea ice thickness data, especially in near real time (NRT), will enable evaluation and improved skill in the prediction of sea ice thickness distributions by climate models. Although it is possible to calculate Arctic sea ice thickness using measurements acquired by CryoSat-2, the latency of the nominal data set typically exceeds 1-2 months due to the time required to determine precise satellite orbits. The second part of this presentation will introduce our new NRT Arctic sea ice thickness dataset, based on preliminary orbits, which provides Arctic-wide sea ice thickness estimates just three days after acquisition from the satellite and is publicly available. A NRT sea ice thickness estimate is delivered, on average, within 64 km of each location in the Arctic every 14 days.
Rachel Tilling
University College London
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3:30 pm |
Increase in the Frequency and Extent of Sub-Ice Phytoplankton Blooms in the Arctic OceanIncrease in the Frequency and Extent of Sub-Ice Phytoplankton Blooms in the Arctic Ocean
Christopher Horvat, Harvard University, USA, bndnchrs [at] gmail.com
Sarah Iams, Harvard University, USA, siams [at] seas.harvard.edu
David Rees Jones, Oxford University, United Kingdom, David.ReesJones [at] physics.ox.ac.uk
David Schroeder, CPOM, University of Reading, United Kingdom, d.schroeder [at] reading.ac.uk
Daniela Flocco, CPOM, University of Reading, United Kingdom, d.flocco [at] reading.ac.uk
Daniel Feltham, CPOM, University of Reading, United Kingdom, d.l.feltham [at] reading.ac.uk
Phytoplankton are a fundamental component of the Arctic ecosystem and carbon cycle. Through their growth and decay, they form the foundation of the oceanic food web and are a sink for atmospheric CO2. Phytoplankton populations undergo periods of exponential growth, known as ``blooms", which occur seasonally in many of the world's oceans. In 2011, a phytoplankton bloom was observed underneath a region of the Arctic fully covered by sea ice, unexpected as sea ice is typically understood to transmit little solar radiation to the ocean below. To investigate the likelihood and location of sub-ice blooms, we develop a critical-depth model for regions of the ice-covered Arctic ocean that incorporates the transmission of solar radiation through regions of sea ice that are covered by melt ponds. We find that favorable conditions for sub-ice blooms exist over a large portion of the modern Arctic. The development of bloom-permitting regions of the ice-covered Arctic, which comprise greater than 30\% of the latitudes above 70N in July has occurred only in the recent two, coinciding with the thinning of Arctic sea ice and an increase in melt pond coverage. Our results demonstrate that these biological events may be both possible and likely in regions previously considered off-limits to photosynthetic activity. Projections of a thinner Arctic sea ice cover in a warming world suggests that the likelihood and extent of sub-ice phytoplankton blooms will increase in the future.
Christopher Horvat
Harvard University
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3:50 pm |
Poster Session with refreshmentsPoster Session with refreshments
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5:30 pm |
Adjourn for day |