2018
DOI: 10.1016/j.cnsns.2018.01.014
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Transport structures in a 3D periodic flow

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Cited by 4 publications
(2 citation statements)
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“…Furthermore, we can demonstrate that the x-axis, {y = 0}, is an attracting S-ridge. Note that s − (x 0 , y 0 ) = −1 + 3y 2 0 < 0 for y 0 = 0, satisfying the attraction criterion, (32). Since ∇s − (x 0 , y 0 ) = [0, 6y 0 ] , then along the xaxis we have ∇s − (x 0 , y 0 )| y0=0 • e − = 0, satisfying the ridge criterion, (33).…”
Section: Two-dimensional Nonlinear Saddle Flowmentioning
confidence: 98%
“…Furthermore, we can demonstrate that the x-axis, {y = 0}, is an attracting S-ridge. Note that s − (x 0 , y 0 ) = −1 + 3y 2 0 < 0 for y 0 = 0, satisfying the attraction criterion, (32). Since ∇s − (x 0 , y 0 ) = [0, 6y 0 ] , then along the xaxis we have ∇s − (x 0 , y 0 )| y0=0 • e − = 0, satisfying the ridge criterion, (33).…”
Section: Two-dimensional Nonlinear Saddle Flowmentioning
confidence: 98%
“…For instance, a 2D flow is divergent in an upwelling region (which drives the particle convergence in garbage patches), while a 3D flow is nondivergent. However, attracting structures (Bettencourt et al, 2012) and transport barriers (Bettencourt et al, 2015;Chang et al, 2018) of 3D particle paths can also emerge inside the ocean. In this way, particles can cluster in specific areas when they are collected at a 2D surface after their sinking journey (Monroy et al, 2017;Eaton and Fessler, 1994), as is also measured at the ocean subsurface (Mitchell et al, 2008;Logan and Wilkinson, 1990).…”
Section: Introductionmentioning
confidence: 99%