2015
DOI: 10.1002/2015jc010972
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Pairwise surface drifter separation in the western Pacific sector of the Southern Ocean

Abstract: The Southern Ocean plays a critical role in global climate, yet the mixing properties of the circulation in this part of the ocean remain poorly understood. Here dispersion in the vicinity of the Southern Antarctic Circumpolar Current Front, one of the branches of the Antarctic Circumpolar Current, is studied using 10 pairs of surface drifters deployed systematically across the frontal jet and its flanks. Drifter pairs were deployed with an initial separation of 13 m and report their position every hour. The s… Show more

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Cited by 23 publications
(25 citation statements)
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“…The relative dispersion ( D 2 ( t )), which is a benchmark of the mean square separation of particle pairs, is defined by ⟨⟩D2()t.25em=.25em1Ni,jxitxjt2+yityjt2, where i and j refer to each drifter of a pair in the cluster of N drifter pairs and x i , j ( t ), y i , j ( t ) correspond to the coordinates in the Universal Transverse Mercator (UTM) projection at the time t . Typically, pairs or clusters of drifters that are initially separated by a small distance δ and were deployed at a certain time t 0 are used for the analysis. Various studies used “chance pairs,” which are deployed randomly but are simultaneously present in a given study area, to increase the number of drifter pairs for Lagrangian statistics (Dräger‐Dietel et al, 2018; LaCasce, 2010; Lumpkin & Elipot, 2010; Ollitrault et al, 2005; van Sebille et al, 2015). We have avoided the use of chance pairs in this study to overcome the issue of biased dispersion rates that can be produced for submesoscale dispersion (LaCasce & Ohlmann, 2003; Lumpkin & Elipot, 2010).…”
Section: Methodsmentioning
confidence: 99%
“…The relative dispersion ( D 2 ( t )), which is a benchmark of the mean square separation of particle pairs, is defined by ⟨⟩D2()t.25em=.25em1Ni,jxitxjt2+yityjt2, where i and j refer to each drifter of a pair in the cluster of N drifter pairs and x i , j ( t ), y i , j ( t ) correspond to the coordinates in the Universal Transverse Mercator (UTM) projection at the time t . Typically, pairs or clusters of drifters that are initially separated by a small distance δ and were deployed at a certain time t 0 are used for the analysis. Various studies used “chance pairs,” which are deployed randomly but are simultaneously present in a given study area, to increase the number of drifter pairs for Lagrangian statistics (Dräger‐Dietel et al, 2018; LaCasce, 2010; Lumpkin & Elipot, 2010; Ollitrault et al, 2005; van Sebille et al, 2015). We have avoided the use of chance pairs in this study to overcome the issue of biased dispersion rates that can be produced for submesoscale dispersion (LaCasce & Ohlmann, 2003; Lumpkin & Elipot, 2010).…”
Section: Methodsmentioning
confidence: 99%
“…Drijfhout et al 1996, Blanke and Raynaud 1997, Döös et al 2008 and ocean dynamics (e.g. van Sebille et al 2012b, Ypma et al 2015. It is also the most commonly used framework to compute the pathways and distributions of plastic particles in the ocean (e.g.…”
Section: Numerical Simulationsmentioning
confidence: 99%
“…The availability of trajectories of over 22,000 dFADs has revealed a considerable number of probable beaching events, and in many cases their deployment and drift pattern prior to beaching 16 . However, given the high level of fine-scale variability in ocean circulation, small variations in the initial deployment location may lead to varied trajectories and final positions over time 17 . Therefore, quantifying the connectivity between areas of high beaching and the surrounding ocean in a statistically robust way would require observations from many more dFADs.
Figure 1Number of beaching events (1,320 in total) per 1° grid cell across 2016 and 2017.
…”
Section: Introductionmentioning
confidence: 99%