2016
DOI: 10.1063/1.4965026
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An autonomous dynamical system captures all LCSs in three-dimensional unsteady flows

Abstract: Lagrangian coherent structures (LCSs) are material surfaces that shape the finite-time tracer patterns in flows with arbitrary time dependence. Depending on their deformation properties, elliptic and hyperbolic LCSs have been identified from different variational principles, solving different equations. Here we observe that, in three dimensions, initial positions of all variational LCSs are invariant manifolds of the same autonomous dynamical system, generated by the intermediate eigenvector field, ξ(x), of th… Show more

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Cited by 8 publications
(6 citation statements)
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“…A simplified algorithm for computing geodesic LCSs without the use of the direction field is now available 70 , but will not be used in this paper. There is no general extension of geodesic LCS theory to three dimensional flows, but related local variational principles for hyperbolic and elliptic LCSs are now available in three dimensions as well 71,72 . Farazmand & Haller 73 introduce the notion of rotationally coherent LCSs as tubular material surfaces whose elements exhibit identical mean material rotation over a finite time interval [t 0 , t 1 ].…”
Section: Stationary Curves Of the Average Strain: Elliptic Lcssmentioning
confidence: 99%
See 1 more Smart Citation
“…A simplified algorithm for computing geodesic LCSs without the use of the direction field is now available 70 , but will not be used in this paper. There is no general extension of geodesic LCS theory to three dimensional flows, but related local variational principles for hyperbolic and elliptic LCSs are now available in three dimensions as well 71,72 . Farazmand & Haller 73 introduce the notion of rotationally coherent LCSs as tubular material surfaces whose elements exhibit identical mean material rotation over a finite time interval [t 0 , t 1 ].…”
Section: Stationary Curves Of the Average Strain: Elliptic Lcssmentioning
confidence: 99%
“…A simplified algorithm for computing geodesic LCSs without the use of the direction field is now available 70 , but will not be used in this paper. There is no general extension of geodesic LCS theory to three dimensional flows, but related local variational principles for hyperbolic and elliptic LCSs are now available in three dimensions as well 71,72 .…”
Section: Stationary Curves Of the Average Strain: Elliptic Lcssmentioning
confidence: 99%
“…In the next section, we recall the terminology used for the definition of LCSs [13] and OECSs [12] in two-dimensional flows. Variational definitions of LCSs are now available also for threedimensional flows [11], but these definitions do not lead to geodesic problems, and hence are not covered by the computational approach developed here. A similar conclusion holds for OECS definitions obtained as short-term limits of three-dimensional LCS definitions.…”
Section: Null Geodesics and The Computation Of Objective Coherent Structuresmentioning
confidence: 99%
“…In light of this, several methods for the identification of coherent structures (CSs) have been developed [1][2][3][4][5][6]. Only recent mathematical results [7][8][9][10][11][12], however, offer a rigorous and objective (frame-invariant) definition of CSs, uncovering the skeletons behind these wellorganized regions.…”
Section: Introductionmentioning
confidence: 99%
“…While the focus of the present study was on assessing two-dimensional flow structures, the LCS approach can, in principle, be extended to three-dimensional (3D) studies with a vertical component, and LCS methods are increasingly becoming established for 3D applications [20]. Of course, 3D studies will be geometrically more complex and thus can be more challenging to both calculate and visualize.…”
Section: Discussionmentioning
confidence: 99%