10 Additional ReadingWhile it is assumed that the reader has had some exposure to classical dynamical systems concepts, there are a number of good books out there that cover the basic theory. The book by Strogatz (1994) provides an excellent introduction to dynamical systems and chaos and reads very fluently. The text by Verhulst (1996) provides a concise coverage of several main dynamical systems concepts and is also a good introductory book. The very popular book by Guckenheimer and Holmes (1983) is a great reference for dynamical systems theory. Wiggins (1992) and Ottino (1989) are two texts dedicated to studying transport in dynamical systems, and provide a good foundation for understanding this area of dynamical systems. This tutorial
presents a technique for analyzing the global flow geometry
of time-dependent dynamical systems. Since a main source of such systems are fluid flow problems, emphasis was
placed on such applications, however FTLE's and LCS are also
applicable to other systems as well. It has long been recognized that flows with general
time dependence admit emergent patterns which influence the transport of
tracers. These structures are often referred to generically as coherent structures in the fluid mechanics literature. When coherent
structures are studied in terms of quantities derived from fluid
trajectories they are often named Lagrangian coherent structures
(LCS). There is a vast body of literature on coherent structures in
fluid mechanics that we will not attempt to overview here, however
Haller and Yaun (2000) and Provenzale
(1999) provide many
useful references on this subject and discuss some of the various
approaches to understanding transport and are nice papers to read.
As noted by Haller and Yuan (2000), in
much of the literature coherent structures are often vaguely defined, making
the analysis and algorithmic detection of such structures difficult. The
motivation for the series of papers Haller and
Poje(2000), Haller and Yuan
(2000), Haller (2001), and
Haller (2002) was to give a precise definition of LCS for general time
dependent systems defined, perhaps, only over a finite time interval. Haller
provides a hyperbolicity time approach which gives criteria for the existence
of LCS based on invariants of the gradient of the velocity field evaluated
along fluid trajectories. Using this approach, LCS are defined by local extrema
of hyperbolicity time fields. Additionally, for
the sake of comparison, Haller (2001) gives an
alternative definition of LCS in
Sec 2.3 of that paper as local extrema of the
finite-time Lyapunov exponent field. He goes on to show the strong
correspondence between hyperbolicity time fields and
finite-time Lyapunov exponent fields for steady and forced ABC
(Arnold-Beltrami-Childress) flows. While this tutorial does not stick to
Haller's hyperbolicity time approach, these papers helped motivate a lot
of the work that is shown in this tutorial and are recommended.
Doerner et al. (1999) discussed how
level contours of finite-time Lyapunov exponent fields can approximate stable
manifolds for time-independent and periodic systems. In the realm of general
time dependent systems, Pierrehumbert
(1991) and Pierrehumbert
and Yang (1993) used finite-time Lyapunov exponent fields to capture
chaotic mixing regions and transport barriers from atmospheric data. They used
these fields to visualize the existence of structures similar to classical
invariant tori that are well-documented in time-periodic flows. In the paper
by von Hardenberg et al. (2000), a similar approach is used for studying atmospheric
vortices. Many of the ideas covered in this tutorial are explained by
Shadden, et al (2005). There the approach is slightly more formal and
it is not assumed that the dynamical system is smooth. When dealing with
discrete data, the data can often be interpolated to provide an adequate
level of continuity, however most interpolators become increasingly complex
when the level of continuity is increased. Therefore it is not reasonable to
assume that quantities derived from the data will be infinitely smooth, so one
must take care to make sure the quantities are well behaved. Application
of the ideas presented in this tutorial can be found in Voth
et al (2002), Lekien et al (2004), Coulliette,
et al (2004), and Inanc et al
(2005). It should be mentioned
that there exists other methods for locating hyperbolic
structures like LCS using techniques other than FTLE's, such
as uniformly hyperbolic trajectories Yuan
et al (2002), Rogerson
et al (1999), or Poje
and Haller (1999) or exponential dichotomies Coppel
(1978) or Mancho et
al (2003), however, it has been the author's experience
that FTLE's are often better suited when working with
discrete data sets defined over finite time intervals,
however it is interesting to learn about other techniques.
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Comments, Questions or Concerns can be sent to shawn@cds.caltech.edu
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