7 ExamplesThis section contains various examples of Lagrangian Coherent Structures in time-dependent dynamical systems:
To supplement this section, we will later cover in Sec.8 how FTLE fields computed, so the reader will know how the results shown below are produced. If so desired, Sec.8 on the Computation of FTLE's can be read before this section. Additionally, there is publicly available software, MANGEN, which provides a nice array of tools for analyzing dynamical systems defined by discrete data, including the capability to compute FTLE fields. We will show how to download this software, and walk through the computations shown in Sec.7.3 for flow over an airfoil.
7.1 Time-dependent double gyreLet's start with an example similar to the double gyre presented in Sec. 4 by Eq. (13). The flow is described by the stream-function
where
over the domain [0, 2] x [0, 1]. The velocity field is given by
For
Movie 11 shows the
velocity field of the periodic double-gyre for A = 0.1,
Recall that for
Movie 12(a)
shows the FTLE field computed forward in time with an integration
time length of T = 15. Movie 12(b)
shows the FTLE field computed backward in
time with an integration time length of T = -15. Notice that the flow here is
periodic with period
To demonstrate the fact that the LCS shown in Movie 12 are invariant manifolds (or at least quasi-invariant), let us place a material point which moves according to the flow on top of the LCS shown in Movie 12(a). Movie 13 shows the time evolution of the superposition of this material point, denoted by an X, along with the LCS. The initial location of the material point was "eyeballed" to be initially placed on the LCS. From the movie, one can see that the point stays on the LCS when evolved over time. In Movie 13 the LCS is highlighted by plotting the FTLE field using a bi-color contour map in which high values of FTLE's are colored red, and low values colored white. This allows the LCS to be highlighted, and also permits us to better superimpose the evolution of other data. We use similarly skewed contour maps in later examples when showing FTLE fields to help highlight the LCS and keep the rest of the contour plot transparent.
In Movie 14 we now superimpose two parcels of fluid particles, which are initially located on either side of the LCS, with the evolution of the LCS. This movie demonstrates how the LCS acts as a time-dependent separatrix. The parcel which begins to the left of the LCS gets stretched into the left gyre and the parcel that begins on the right side of the LCS gets stretched into the right gyre.
Although the LCS appears to be an invariant manifold from the above movies, we
know from Thm.6.1 that there may be a slight flux across this structure.
Figure 15 shows a
highly refined computation of the LCS and the location of the
Lagrangian tracer shown in Movie 13. The grid spacing that was used for the
computation of FTLE was
To verify Thm. 6.1, the terms in the right-hand-side of Eq. (22)
were computed from a first-order approximation. The
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Page created 04-15-2005, Last updated 04-15-05, Copyright © 2005, All Rights Reserved.