2016
DOI: 10.1017/jfm.2016.208
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On low-frequency variability of the midlatitude ocean gyres

Abstract: This paper studies the large-scale low-frequency variability of the wind-driven midlatitude ocean gyres and their western boundary currents, such as the Gulf Stream or Kuroshio, simulated with the eddy-resolving quasi-geostrophic model. We applied Empirical Orthogonal Functions Analysis to turbulent flow solutions and statistically extracted robust and significant large-scale decadal variability modes concentrated around the eastward jet extension of the western boundary currents. In order to interpret these s… Show more

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Cited by 19 publications
(15 citation statements)
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“…at reference model parameters [8] is characterized by a robust large-scale decadal low-frequency variability (LFV) at ≈17 years and involving coherent meridional shifts of the eastward jet extension separating the gyres. This LFV is driven by transient mesoscale eddies, qualitatively similar to the turbulent oscillator studied by [60,61]; see [62][63][64][65][66][67][68] for alternative theories. Still, there is no clear scale separation between the eddies and large-scale flow, and in fact, the LFV accounts for a relatively small fraction of the total variability, as demonstrated below in the detailed DAH analysis.…”
Section: Oceanic Datasetsupporting
confidence: 64%
“…at reference model parameters [8] is characterized by a robust large-scale decadal low-frequency variability (LFV) at ≈17 years and involving coherent meridional shifts of the eastward jet extension separating the gyres. This LFV is driven by transient mesoscale eddies, qualitatively similar to the turbulent oscillator studied by [60,61]; see [62][63][64][65][66][67][68] for alternative theories. Still, there is no clear scale separation between the eddies and large-scale flow, and in fact, the LFV accounts for a relatively small fraction of the total variability, as demonstrated below in the detailed DAH analysis.…”
Section: Oceanic Datasetsupporting
confidence: 64%
“…Specific modes of variability have been identified in various idealized ocean models. A turbulent oscillator mode was proposed by Berloff et al (2007b) with a rough time scale of 12 years, and has been found in other quasigeostrophic models as well (e.g., Shevchenko et al 2016). This mode is characterized by changes to the magnitude and position of the oceanic jet in the western boundary current separation region.…”
Section: Introductionmentioning
confidence: 65%
“…Also a small set of modes should be sufficient in order to assure feasibility. However, dynamical modes are typically constructed via generalized eigenproblems (e.g., linear instability modes; Dijkstra 2005;Berloff 2005b;Shevchenko et al 2016) or optimization problems (e.g., Lyapunov vectors, CNOPs; Dijkstra 2013; Dijkstra and Viebahn 2015) and, hence, are generally expensive to compute, if at all.…”
Section: Dynamical Spatial Mode Representation Of the Eddy Forcingmentioning
confidence: 99%
“…In this case, the LFV is not a single-mode pattern, but rather a coherent pattern phenomenon consisting of a large number of short period phase-related eigenmodes interacting with each other. We note that this can apply to both (high resolution) statistical eigenmodes like EOFs (Gille and Kelly 1996) and linear eigenmodes on a background flow (Shevchenko et al 2016). Obviously, the small-scale structures of the dynamical modes are not resolvable on a low-resolution model grid.…”
Section: Introductionmentioning
confidence: 97%
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