Ice-Cover and Ice-Ridge Contributions to the Freshwater Contents of Hudson Bay and Foxe Basin

Runoff and precipitation add 65 cm of fresh water to Hudson Bay annually. The ice cover does not account for a new contribution of fresh water over a one-year period; however, on weekly time scales, it contributes as much or more than runoff. The maximum thickness of ice averaged over the bay is 160 cm and represents a 140 cm layer of fresh water when sublimation is accounted for. This fresh water is twice as large as the amount annually brought in by runoff and precipitation and is added to the surface layer in the spring and removed from the surface layer in the fall. Freshwater budgets of Hudson Bay and Foxe Basin indicate up to 90% more ice is produced than indicated by ice thickness data. Part of this difference can be attributed to the ice accumulated in ice ridges, which for Hudson Bay accounts for 25 cm of ice and as much as 58 cm of ice for Foxe Basin, where extreme rough ice conditions occur.Key words: Hudson Bay, Foxe Basin, ice cover, ice ridges, freshwater contentMots clés: baie d’Hudson, bassin de Foxe, couverture de glace, crêtes de glace, volume d’eau douc

What is the fate of the river waters of Hudson Bay?

Author Posting. © The Author(s), 2011. This is the author's version of the work. It is posted here by permission of Elsevier B.V. for personal use, not for redistribution. The definitive version was published in Journal of Marine Systems 88 (2011): 352-361, doi:10.1016/j.jmarsys.2011.02.004.We examine the freshwater balance of Hudson and James bays, two shallow and fresh seas that annually receive 12% of the pan- Arctic river runoff. The analyses use the results from a 3–D sea ice-ocean coupled model with realistic forcing for tides, rivers, ocean boundaries, precipitation, and winds. The model simulations show that the annual freshwater balance is essentially between the river input and a large outflow toward the Labrador shelf. River waters are seasonally exchanged from the nearshore region to the interior of the basin, and the volumes exchanged are substantial (of the same order of magnitude as the annual river input). This lateral exchange is mostly caused by Ekman transport, and its magnitude and variability are controlled by the curl of the stress at the surface of the basin. The average transit time of the river waters is 3.0 years, meaning that the outflow is a complex mixture of the runoff from the three preceding years.We thank NSERC and the Canada Research Chairs program for funding. FS acknowledges support from NSF OCE-0751554 and ONR N00014-08-10490

A conceptual model of an Arctic sea

Author Posting. © American Geophysical Union, 2012. This article is posted here by permission of American Geophysical Union for personal use, not for redistribution. The definitive version was published in Journal of Geophysical Research 117 (2012): C06010, doi:10.1029/2011JC007652.We propose a conceptual model for an Arctic sea that is driven by river runoff, atmospheric fluxes, sea ice melt/growth, and winds. The model domain is divided into two areas, the interior and boundary regions, that are coupled through Ekman and eddy fluxes of buoyancy. The model is applied to Hudson and James Bays (HJB, a large inland basin in northeastern Canada) for the period 1979–2007. Several yearlong records from instruments moored within HJB show that the model results are consistent with the real system. The model notably reproduces the seasonal migration of the halocline, the baroclinic boundary current, spatial variability of freshwater content, and the fall maximum in freshwater export. The simulations clarify the important differences in the freshwater balance of the western and eastern sides of HJB. The significant role played by the boundary current in the freshwater budget of the system, and its sensitivity to the wind-forcing, are also highlighted by the simulations and new data analyses. We conclude that the model proposed is useful for the interpretation of observed data from Arctic seas and model outputs from more complex coupled/climate models.We thank NSERC and the Canada Research Chairs program for funding. FS acknowledges support from NSF OCE–0927797 and ONR N00014-08-10490.2012-12-2

Measuring ice thickness with EISFlowTM, a fixed-mounted helicopter electromagneticlaser system

ABSTRACT A helicopter-borne ice thickness sensor, mounted on the nose of an MBB B0105 helicopter, was developed for the Canadian Coast Guard in support of its ice breaking operations. The sensor utilises low-frequency electromagnetic induction measurements, coupled with a precise laser altimeter, to measure snow plus ice thickness over seawater to centimetre-level accuracy with the helicopter skids on the ice. The system can also be operated in a profiling mode, yielding similar mean ice thickness accuracy over the sensor's footprint. For 1 m thick ice the footprint's diameter increases from 6 m for soft-landing to 12 m for profiling mode of operations. Soft-landing mode of observations are made with the helicopter's skids on the ice but not with the helicopter's weight on the ice

Summer Sea Ice Concentration, Motion, and Thickness Near Areas of Proposed Offshore Oil and Gas Development in the Canadian Beaufort Sea – 2009

This study was motivated by the potential development of offshore oil exploration leases in the Canadian Southern Beaufort Sea, an area within the Inuvialuit Settlement Region. Sea ice concentration, extent, motion, and thickness data are vital to the success of potential oil operations in this region, and relevant data cannot be gleaned from larger-scale hemispheric studies. We therefore undertook regionally specific sea ice analyses in the southern Beaufort Sea during the summer drilling season (July, August, and September) in 2009 and over the long-term (1996 – 2010). On average, the Canadian oil lease areas contain mostly old sea ice during the drilling season and have not experienced significant decreasing trends in total or old sea ice. The average sea ice motion in the region for the period was anti-cyclonic at 20 – 25 cm·s-1, acting to transport sea ice southward toward the lease areas. Summer 2009 was used as a case study of regional ice concentration, motion, and thickness and to compare September sea ice thickness measurements to data collected in April 2009. In the summer of 2009, old sea ice was the predominant ice type in the lease areas. Sea ice motion was anti-cyclonic and faster than the long-term average, reaching 60 cm·s-1 west of Banks Island and across the north end of the lease areas. September 2009 sea ice thickness (mean = 1.03 m, σ = 0.97 m) was modal about the 0.20 – 0.29 m thickness bin. The sea ice thickness distri­bution was spatially variable, with the thickest ice occurring at the north end of the study area, in an area dominated by high old ice concentrations. Ice thicknesses greater than 10 m (the upper limit our instruments could measure) were encountered. Thinner sea ice predominated at the periphery of the core Beaufort Sea multi-year pack. Near the oil lease areas, the sea ice thickness distributions were shifted left on the histogram in comparison to those farther north, resulting in a greater proportion of relatively thick sea ice due to the thermodynamic loss of thinner (< 1.5 m) first-year ice during its southward movement. After enduring a summer’s melt, however, this thicker ice at the south end of the study region had thinned in comparison to the ice at the north end.La présente étude a été motivée par la mise en valeur potentielle des concessions d’exploration pétrolière au large de la mer de Beaufort, dans la partie sud canadienne, un endroit qui fait partie de la région désignée des Inuvialuit. Les données relatives à la concentration, à l’étendue, au déplacement et à l’épaisseur de la glace de mer sont essentielles à la réussite de l’exploitation éventuelle du pétrole dans cette région, et les données pertinentes ne peuvent être dépouillées à partir d’études hémisphériques réalisées à grande échelle. Par conséquent, nous avons entrepris de faire des analyses particulièrement régionales de la glace de mer du sud de la mer de Beaufort pendant la saison de forage d’été (juillet, août et septembre) en 2009 de même que sur une plus longue période (1996-2010). En moyenne, les régions visées par les concessions pétrolières canadiennes renferment principalement de la vieille glace de mer pendant la saison de forage, et elles n’enregistrent pas d’importantes tendances à la baisse sur le plan de l’ensemble de la glace de mer ou de la vieille glace de mer. Dans la région, le déplacement moyen de la glace de mer pendant la période était anticyclonique à 20 25 cm·s-1, ce qui avait pour effet de transporter la glace de mer vers le sud et vers les concessions. L’été 2009 nous a servi d’étude de cas en matière de concentration, de déplacement et d’épaisseur de la glace régionale, et nous a permis de comparer les mesures de l’épaisseur de la glace de mer de septembre aux données recueillies en avril 2009. À l’été 2009, la vieille glace de mer représentait le type de glace prédominant dans les concessions. Le déplacement de la glace de mer était anticyclonique et se faisait plus vite que la moyenne à long terme, atteignant ainsi 60 cm·s-1 à l’ouest de l’île Banks et à la hauteur du nord de la zone de concessions. En septembre 2009, l’épaisseur de la glace de mer (moyenne = 1,03 m, σ = 0,97 m) était modale à la hauteur de la classe de l’épaisseur 0,20 – 0,29 m. La répartition de l’épaisseur de la glace de mer variait en fonction de l’emplacement, la glace la plus épaisse se trouvant du côté nord de la région étudiée, dans une zone dominée par de fortes concentrations de vieille glace. La glace atteignait des épaisseurs de plus de 10 m (la limite maximale que nos instruments pouvaient mesurer) par endroits. Une glace de mer plus mince prédominait la périphérie du noyau de la banquise pluriannuelle de la mer de Beaufort. Près de la zone de concessions pétrolières, les répartitions d’épaisseurs de glace de mer se sont déplacées vers la gauche sur l’histogramme comparativement à celles plus au nord, ce qui a donné une plus grande proportion de glace de mer relativement épaisse en raison de la perte thermodynamique de la glace plus mince de première année (< 1,5 m) pendant son déplacement vers le sud. Cependant, après avoir enduré la fonte d’un été, la glace plus épaisse du côté sud de la région à l’étude s’était amincie compara­tivement à la glace se trouvant du côté nord

Effects of friction and surface tide angle of incidence on the coastal generation of internal tides

For the generation of internal waves by long surface waves, the normal-mode equations and solutions that satisfy the boundary conditions in a two-layer system are found analytically. Frictional effects decrease the amplitude of an internal wave over the shelf, changing it from a standing wave to a wave that progresses coastward and decreases the interference on the amplitude of the offshore progressive wave traveling seaward. Model studies, using a two-layer system of fresh water and saline water in a 9.9-m-long channel, gave favorable results relative to the theoretical results

The outflow from Hudson Strait and its contribution to the Labrador Current

Author Posting. © Elsevier B.V., 2008. This is the author's version of the work. It is posted here by permission of Elsevier B.V. for personal use, not for redistribution. The definitive version was published in Deep Sea Research Part I: Oceanographic Research Papers 55 (2008): 926-946, doi:10.1016/j.dsr.2008.03.012.Hudson Strait delivers a large amount of fresh water to the subpolar North Atlantic due to a large riverine input into the upstream Hudson Bay System and to the rerouting of Arctic Ocean waters. The fresh waters flowing out of Hudson Strait feed the Labrador Current, a current that has a significant impact on the climate and ecosystem of the entire northeastern seaboard. The lack of measurements from the strait have, until recently, made it difficult to determine the relative contribution of Hudson Strait to the properties and variability of the Labrador Current compared to other sources. This study describes the first year round observations of the outflow as obtained from a moored array deployed midstrait from August 2004 to 2005, and from a highresolution hydrographic section conducted in September of 2005. The outflow from Hudson Strait has the structure of a buoyant boundary current spread across the sloping topography of its southern edge. The variability in the flow is dominated by the extreme semidiurnal tides and by vigorous, mostly barotropic, fluctuations over several days. The fresh water export is seasonally concentrated between June and March with a peak in NovemberDecember, consistent with the seasonal riverine input and seaice melt. It is highly variable on weekly timescales due to synchronous salinity and velocity variations. The estimated volume and liquid fresh water transports during 20042005 are respectively of 11.2 Sv and 7888 (2829) mSv relative to a salinity of 34.8 (33). This implies that the Hudson Strait outflow accounts for approximately 15% of the volume and 50% of the fresh water transports of the Labrador Current. This larger than previously estimated contribution is partially due to the recycling, within the Hudson Bay System, of relatively fresh waters that flow into Hudson Strait, along its northern edge. It is speculated that the source of this inflow is the outflow from Davis Strait.Straneo acknowledges support from the Woods Hole Oceanographic Institution's Ocean and Climate Change Institute and the Comer Foundation, in particular, as well as support for NSF OCE0629411. Support to FJS from NSERC Research Grant and the Canadian Program on Energy Research and Development