2016
DOI: 10.3402/polar.v35.30778
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Lagrangian analysis of sea-ice dynamics in the Arctic Ocean

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Cited by 7 publications
(16 citation statements)
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“…Indeed, ignoring boundary effects, for a spherical particle that is completely immersed in the water τ = a 2 ρ/3µ, 19,26 while τ = a 2 ρ a /3µ a ≡ (ρ a /ργ) · (a 2 ρ/3µ) if the particle is fully (17), lim δ→∞ τ = 0. But this limit, as clarified above, is outside the domain of validity of the Maxey-Riley set (5) or its reduced form (12). It turns out that what really matters once the theory is confronted with observations is that (17) makes τ to decay at a faster rate with increasing δ than k = k a = 1, which corresponds to setting the projected length of the submerged (resp., emerged) particle piece to be equal to the submerged depth (resp., emerged height).…”
Section: Parameter Specificationmentioning
confidence: 97%
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“…Indeed, ignoring boundary effects, for a spherical particle that is completely immersed in the water τ = a 2 ρ/3µ, 19,26 while τ = a 2 ρ a /3µ a ≡ (ρ a /ργ) · (a 2 ρ/3µ) if the particle is fully (17), lim δ→∞ τ = 0. But this limit, as clarified above, is outside the domain of validity of the Maxey-Riley set (5) or its reduced form (12). It turns out that what really matters once the theory is confronted with observations is that (17) makes τ to decay at a faster rate with increasing δ than k = k a = 1, which corresponds to setting the projected length of the submerged (resp., emerged) particle piece to be equal to the submerged depth (resp., emerged height).…”
Section: Parameter Specificationmentioning
confidence: 97%
“…Examples of relevant aspects include clustering at the center of the subtropical gyres 18,19 , phenomenon supported on measurements of plastic debris concentration 7 and the analysis of undrogued drifter trajectories 18,19 , or the role of mesoscale eddies as attractors or repellers of inertial particles depending on the polarity of the eddies and the buoyancy of the particles 19,27,28 despite the Lagrangian resilience of their boundaries [48][49][50][51] , which is also backed on observations 52 . The cited phenomena, which act on quite different timescales, all require both O(1) and O(τ ) terms in (12) for their description 18,19,27,28 consistent with the slow manifold M τ in (14), rather than the critical M 0 , controlling the time-asymptotic dynamics of the τ → 0 limit of the Maxey-Riley set (5).…”
Section: Clarification Of the Maxey-riley Setmentioning
confidence: 99%
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“…Understanding these dynamics is especially important in the context of future trends towards thinner sea ice and ice-free summers, and changes in the extent of ice-free areas, ice movement patterns in polar regions and resulting changes in ocean circulation transport. Changes caused by the shift from multiyear ice extent to first-year ice might result in the tendency of sea ice floes to diverge from the main drift pattern such as the Transpolar Drift (Szanyi et al 2016), with complex effects on exchange processes of any contaminants between the Exclusive Economic Zones of the various Arctic nations (Newton et al 2017). 4.10.…”
Section: Ice Formation Melting and Driftmentioning
confidence: 99%