2022
DOI: 10.1029/2021jc017963
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Landfast Ice Controls on Turbulence in Antarctic Coastal Seas

Abstract: Knowledge of the ocean surface layer beneath Antarctic landfast ice is sparse. In this article surface layer turbulent and fine structure are quantified with and without landfast ice at the same West Antarctic Peninsula location. Landfast ice reduced turbulence levels locally to an order of magnitude less than ice‐free values, and near‐inertial energy and sub‐inertial tidal energy levels to less than half their ice‐free values. Vertical turbulent heat and nutrient fluxes were, respectively, 6 and 10 times grea… Show more

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Cited by 6 publications
(12 citation statements)
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“…They are consistently lower than those observed in shear-driven ice shelf-ocean boundary layers (Davis & Nicholls, 2019) or beneath fast ice (Inall et al, 2022), and tend to indicate that despite the tidal forcing, the region of the cavity sampled by ALR is relatively quiescent (at least during neap tides). Over the depth range covered by the vehicle, there is no evidence of ε and χ scaling with the mean flow speed, or of an increase in mixing at the ice front where the flow is required…”
Section: Microstructurementioning
confidence: 77%
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“…They are consistently lower than those observed in shear-driven ice shelf-ocean boundary layers (Davis & Nicholls, 2019) or beneath fast ice (Inall et al, 2022), and tend to indicate that despite the tidal forcing, the region of the cavity sampled by ALR is relatively quiescent (at least during neap tides). Over the depth range covered by the vehicle, there is no evidence of ε and χ scaling with the mean flow speed, or of an increase in mixing at the ice front where the flow is required…”
Section: Microstructurementioning
confidence: 77%
“…The RSI MicroRider package had four microstructure probes sampling at a rate of 512 Hz: two orthogonally positioned shear probes that provide an estimate of the rate of turbulent kinetic energy dissipation (TKE; ε), and two thermistor probes that provide an estimate of the rate of thermal variance dissipation (χ). The microstructure data were processed following standard methods (e.g., Inall et al., 2022; Kimura et al., 2016; Piccolroaz et al., 2021; Scott et al., 2021). Under the assumption of small‐scale isotropy, ε can be estimated as normalε=152ν〈〉uz2=152normalν0kIψS(k)0.25emdk, ${\varepsilon}=\frac{15}{2}\nu \left\langle {\left(\frac{{\partial u}^{\prime }}{\partial z}\right)}^{2}\right\rangle =\frac{15}{2}{\nu}\int \nolimits_{0}^{{k}_{I}}{\psi }_{S}(k)\,dk,$ where ν is the temperature‐dependant kinematic viscosity of seawater and 〈〉()u/z2 $\left\langle {\left({\partial u}^{\prime }/\partial z\right)}^{2}\right\rangle $ is the variance of the velocity shear fluctuations perpendicular to ALR's path (Osborn, 1974) derived from integrating the velocity shear spectrum ψS ${\psi }_{S}$ in wavenumber space k $k$ up to kI ${k}_{I}$.…”
Section: Autosub Long Range Observations and Methodsmentioning
confidence: 99%
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“…Buoyancy forcing occurs through heat loss and sea ice production in winter; combined with restratification in summer, this sets the seasonal cycle of water column stability. Winds and tides exert a year-round destratifying influence, modulated by sea ice and influenced by topography ( 18 ). Mixing has been incorporated into ocean and climate models using representations or parameterizations of these processes.…”
Section: Introductionmentioning
confidence: 99%