Academic literature on the topic 'Glacial fjord Circulation'

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Journal articles on the topic "Glacial fjord Circulation"

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Zhao, Ken X., Andrew L. Stewart, and James C. McWilliams. "Geometric Constraints on Glacial Fjord–Shelf Exchange." Journal of Physical Oceanography 51, no. 4 (2021): 1223–46. http://dx.doi.org/10.1175/jpo-d-20-0091.1.

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AbstractThe oceanic connections between tidewater glaciers and continental shelf waters are modulated and controlled by geometrically complex fjords. These fjords exhibit both overturning circulations and horizontal recirculations, driven by a combination of water mass transformation at the head of the fjord, variability on the continental shelf, and atmospheric forcing. However, it remains unclear which geometric and forcing parameters are the most important in exerting control on the overturning and horizontal recirculation. To address this, idealized numerical simulations are conducted usin
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Bao, Weiyang, and Carlos Moffat. "Impact of shallow sills on circulation regimes and submarine melting in glacial fjords." Cryosphere 18, no. 1 (2024): 187–203. http://dx.doi.org/10.5194/tc-18-187-2024.

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Abstract. The increased melting and rapid retreat of marine-terminating glaciers is a key contributor to sea-level rise. In glacial fjords with shallow sills common in Patagonia, Alaska, and other systems, these bathymetric features can act as a first-order control on the dynamics. However, our understanding of how this shallow bathymetry interacts with the subglacial discharge from the glacier and impacts the fjord circulation, water properties, and rates of submarine melting is limited. To address this gap, we conduct idealized numerical simulations using a coupled plume–ocean fjord model sp
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Santos-Garcia, Marta, Raja S. Ganeshram, Robyn E. Tuerena, et al. "Nitrate isotope investigations reveal future impacts of climate change on nitrogen inputs and cycling in Arctic fjords: Kongsfjorden and Rijpfjorden (Svalbard)." Biogeosciences 19, no. 24 (2022): 5973–6002. http://dx.doi.org/10.5194/bg-19-5973-2022.

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Abstract. Ongoing climate change in the Arctic has caused tidewater glaciers to retreat while increasing the discharge of freshwater and terrestrial material into fjords. This can affect both nutrient inputs and cycling within the fjord systems. In particular, tidewater glaciers and the presence of associated subglacial meltwater plumes can have a large impact on fjord circulation and biogeochemistry. In this study, we assess the influence of tidewater glaciers on nitrogen inputs and cycling in two fjords in Svalbard during the summer using stable isotopic analyses of dissolved nitrate (δ15N a
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Abib, Nicole, David A. Sutherland, Rachel Peterson, et al. "Ice mélange melt changes observed water column stratification at a tidewater glacier in Greenland." Cryosphere 18, no. 10 (2024): 4817–29. http://dx.doi.org/10.5194/tc-18-4817-2024.

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Abstract. Glacial fjords often contain ice mélange, a frozen conglomeration of icebergs and sea ice, which has been postulated to influence both glacier dynamics and fjord circulation through coupled mechanical and thermodynamic processes. Ice mélange meltwater can alter stratification of the water column by releasing cool fresh water across a range of depths in the upper layer of the fjord. This meltwater input can subsequently modify the depth at which the subglacial discharge plume reaches neutral buoyancy and therefore the underlying buoyancy-driven fjord circulation and heat exchange with
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Ross, Lauren, Iván Pérez-Santos, Brigitte Parady, Leonardo Castro, Arnoldo Valle-Levinson, and Wolfgang Schneider. "Glacial Lake Outburst Flood (GLOF) Events and Water Response in A Patagonian Fjord." Water 12, no. 1 (2020): 248. http://dx.doi.org/10.3390/w12010248.

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As a result of climate change, the frequency of glacial lake outburst floods (GLOF) is increasing in Chilean Patagonia. Yet, the impacts of the flood events on the physics and biology of fjords is still unknown. Current velocities, density, in-situ zooplankton samples, and volume backscatter (Sv) derived from an acoustic profiler were used to explore the response of circulation and zooplankton abundance in a Patagonian fjord to GLOF events in 2010 and 2014. Maximum Sv was found both during the GLOFs and in late winter to early spring of 2010 and the fall and summer of 2014. The increase in Sv
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Straneo, Fiammetta, Ruth G. Curry, David A. Sutherland, et al. "Impact of fjord dynamics and glacial runoff on the circulation near Helheim Glacier." Nature Geoscience 4, no. 5 (2011): 322–27. http://dx.doi.org/10.1038/ngeo1109.

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Beaird, Nicholas, Fiammetta Straneo, and William Jenkins. "Characteristics of meltwater export from Jakobshavn Isbræ and Ilulissat Icefjord." Annals of Glaciology 58, no. 74 (2017): 107–17. http://dx.doi.org/10.1017/aog.2017.19.

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ABSTRACT Jakobshavn Isbræ, which terminates in Ilulissat Icefjord, has undergone rapid retreat and is currently the largest contributor to ice-sheet mass loss among Greenland's marine terminating glaciers. Accelerating mass loss is increasing fresh water discharge to the ocean, which can feed back on ice melt, impact marine ecosystems and potentially modify regional and larger scale ocean circulation. Here we present hydrographic observations, including inert geochemical tracers, that allow the first quantitative description of the glacially-modified waters exported from the Jakobshavn/Icefjor
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Williams, Christopher N., Stephen L. Cornford, Thomas M. Jordan, et al. "Generating synthetic fjord bathymetry for coastal Greenland." Cryosphere 11, no. 1 (2017): 363–80. http://dx.doi.org/10.5194/tc-11-363-2017.

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Abstract. Bed topography is a critical boundary for the numerical modelling of ice sheets and ice–ocean interactions. A persistent issue with existing topography products for the bed of the Greenland Ice Sheet and surrounding sea floor is the poor representation of coastal bathymetry, especially in regions of floating ice and near the grounding line. Sparse data coverage, and the resultant coarse resolution at the ice–ocean boundary, poses issues in our ability to model ice flow advance and retreat from the present position. In addition, as fjord bathymetry is known to exert strong control on
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Cowan, Ellen A. "Meltwater and tidal currents: Controls on circulation in a small glacial fjord." Estuarine, Coastal and Shelf Science 34, no. 4 (1992): 381–92. http://dx.doi.org/10.1016/s0272-7714(05)80077-0.

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Heuzé, Céline, Anna Wåhlin, Helen L. Johnson, and Andreas Münchow. "Pathways of Meltwater Export from Petermann Glacier, Greenland." Journal of Physical Oceanography 47, no. 2 (2017): 405–18. http://dx.doi.org/10.1175/jpo-d-16-0161.1.

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AbstractIntrusions of Atlantic Water cause basal melting of Greenland’s marine-terminating glaciers and ice shelves, such as that of Petermann Glacier, in northwest Greenland. The fate of the resulting glacial meltwater is largely unknown. It is investigated here, using hydrographic observations collected during a research cruise in Petermann Fjord and adjacent Nares Strait onboard icebreaker (I/B) Oden in August 2015. A three end-member mixing method provides the concentration of Petermann ice shelf meltwater. Meltwater from Petermann is found in all of the casts in adjacent Nares Strait, wit
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Dissertations / Theses on the topic "Glacial fjord Circulation"

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Carroll, Dustin. "Modeling Circulation Dynamics and Submarine Melt in Greenland Fjords." Thesis, University of Oregon, 2017. http://hdl.handle.net/1794/22626.

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Meltwater accumulated on the Greenland Ice Sheet drains to glacier beds, discharging into fjords hundreds of meters below sea level. The injection of meltwater at depth generates an upwelling plume that entrains warm ocean water as it rises along the terminus, increasing submarine melt and driving a fjord-scale exchange flow. However, due to sparse ocean-glacier observations, we lack a process understanding of how plumes control fjord circulation and submarine melt. Combining numerical modeling, theory, and observations, this dissertation investigates near-glacier plume dynamics, the influence
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Book chapters on the topic "Glacial fjord Circulation"

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"Hudson River Fishes and their Environment." In Hudson River Fishes and their Environment, edited by Alan F. Blumberg and Ferdi L. Hellweger. American Fisheries Society, 2006. http://dx.doi.org/10.47886/9781888569827.ch2.

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<em>Abstract.</em>—The Hudson River Estuary can be classified as a drowned river valley, partially mixed, tidally dominated estuary. Originally, it had a fjord-like morphology as a result of glacial scour which filled in over the past 3,000 years with river sediments. The hydrodynamics of the estuary are best described by the drivers of circulation, including the upstream river inflows, the oceanographic conditions at the downstream end, and meteorological conditions at the water surface and the response of the waters to these drivers in terms of tides and surges, currents, temperature, and salinity. Freshwater inflow is predominantly from the Mohawk and Upper Hudson rivers at Troy (average flow = 400 m<sup>3</sup>/s, highest in April, lowest in August). At the downstream end at the Battery the dominant tidal constituent is the semidiurnal, principal lunar constituent (the M<sub>2</sub> tide), with an evident spring/neap cycle. The amplitude of the tide is highest at the Battery (67 cm), lower at West Point (38 cm), and higher again at Albany (69 cm), a function of friction, geometry, and wave reflection. Meteorological events can also raise the water surface elevation at the downstream end and propagate into the estuary. Freshwater pulses can raise the water level at the upstream end and propagate downstream. Tidal flows are typically about an order of magnitude greater than net flows. The typical tidal excursion in the Hudson River Estuary is 5–10 km, but it can be as high as 20 km. Temperature varies seasonally in response to atmospheric heating and cooling with a typical August maximum of 25°C and January-February minimum of 1°C. Power plants cause local heating. The salinity intrusion varies with the tide and amount of upstream freshwater input. The location of the salt front is between Yonkers and Tappan Zee in the spring and just south of Poughkeepsie in the summer. Vertical salinity stratification exists in the area of salt intrusion setting up an estuarine circulation. The effect of wind is limited due to a prevailing wind direction perpendicular to the main axis and the presence of cliffs and hills. Dispersive processes include shear dispersion and tidal trapping, resulting in an overall longitudinal dispersion coefficient of 3–270 m<sup>2</sup>/s. The residence or flushing time in the freshwater reach is less than 40 d in the spring and about 200 d in the summer. In the area of salt intrusion, it is about 8 d.
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"Hudson River Fishes and their Environment." In Hudson River Fishes and their Environment, edited by Alan F. Blumberg and Ferdi L. Hellweger. American Fisheries Society, 2006. http://dx.doi.org/10.47886/9781888569827.ch2.

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Abstract:
<em>Abstract.</em>—The Hudson River Estuary can be classified as a drowned river valley, partially mixed, tidally dominated estuary. Originally, it had a fjord-like morphology as a result of glacial scour which filled in over the past 3,000 years with river sediments. The hydrodynamics of the estuary are best described by the drivers of circulation, including the upstream river inflows, the oceanographic conditions at the downstream end, and meteorological conditions at the water surface and the response of the waters to these drivers in terms of tides and surges, currents, temperature, and salinity. Freshwater inflow is predominantly from the Mohawk and Upper Hudson rivers at Troy (average flow = 400 m<sup>3</sup>/s, highest in April, lowest in August). At the downstream end at the Battery the dominant tidal constituent is the semidiurnal, principal lunar constituent (the M<sub>2</sub> tide), with an evident spring/neap cycle. The amplitude of the tide is highest at the Battery (67 cm), lower at West Point (38 cm), and higher again at Albany (69 cm), a function of friction, geometry, and wave reflection. Meteorological events can also raise the water surface elevation at the downstream end and propagate into the estuary. Freshwater pulses can raise the water level at the upstream end and propagate downstream. Tidal flows are typically about an order of magnitude greater than net flows. The typical tidal excursion in the Hudson River Estuary is 5–10 km, but it can be as high as 20 km. Temperature varies seasonally in response to atmospheric heating and cooling with a typical August maximum of 25°C and January-February minimum of 1°C. Power plants cause local heating. The salinity intrusion varies with the tide and amount of upstream freshwater input. The location of the salt front is between Yonkers and Tappan Zee in the spring and just south of Poughkeepsie in the summer. Vertical salinity stratification exists in the area of salt intrusion setting up an estuarine circulation. The effect of wind is limited due to a prevailing wind direction perpendicular to the main axis and the presence of cliffs and hills. Dispersive processes include shear dispersion and tidal trapping, resulting in an overall longitudinal dispersion coefficient of 3–270 m<sup>2</sup>/s. The residence or flushing time in the freshwater reach is less than 40 d in the spring and about 200 d in the summer. In the area of salt intrusion, it is about 8 d.
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Conference papers on the topic "Glacial fjord Circulation"

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Storms, J. E. A., M. Schoenmakers, L. Hansen, N. Waldmann, and A. Beylich. "Understanding Glacier-induced Wind-driven Circulation Patterns in Strynevatnet Fjord (Norway) and their Implications for Fjord-infill Patterns." In Second Conference on Forward Modelling of Sedimentary Systems. EAGE Publications BV, 2016. http://dx.doi.org/10.3997/2214-4609.201600362.

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