# Difference between revisions of "Periodic orbits"

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[[File:DblPendShadowing.png|400px|thumb|right|Shadowing of two periodic orbits (red and green) leads to a longer one (blue).]] | [[File:DblPendShadowing.png|400px|thumb|right|Shadowing of two periodic orbits (red and green) leads to a longer one (blue).]] | ||

Apparently complex dynamics can originate from a small set of dynamically important recurring patterns. | Apparently complex dynamics can originate from a small set of dynamically important recurring patterns. | ||

− | The image to the right shows two | + | The image to the right shows two recurring patterns (green,red) that exist in the double pendulum setup. |

(A simple android application and screenshots of the setup can be found | (A simple android application and screenshots of the setup can be found | ||

[https://play.google.com/store/apps/details?id=org.openpipeflow.doubledoublependulum HERE]; | [https://play.google.com/store/apps/details?id=org.openpipeflow.doubledoublependulum HERE]; | ||

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The lines are the time-trace of the lower pendulum, i.e. the state of the system has been projected onto (x,y)=(position of lower pendulum). | The lines are the time-trace of the lower pendulum, i.e. the state of the system has been projected onto (x,y)=(position of lower pendulum). | ||

− | As the state of a system changes in time its 'state-vector' traces out a trajectory | + | As the state of a system changes in time, its 'state-vector' traces out a trajectory. If the state returns to a state that has been seen before, then it traces out a closed 'periodic orbit'. |

− | + | Observe that the longer orbit (blue) in the example can be considered to be constructed from 'shadowing' of the two simpler orbits. | |

+ | To understand a lot about the dynamics it is sufficient to find the short periodic orbits. These we might call our 'alphabet', out of which infinitely many 'words', i.e. longer orbits, may be constructed. | ||

An excellent (graduate level) free text on periodic orbits can be found at | An excellent (graduate level) free text on periodic orbits can be found at |

## Revision as of 09:00, 27 June 2016

Apparently complex dynamics can originate from a small set of dynamically important recurring patterns. The image to the right shows two recurring patterns (green,red) that exist in the double pendulum setup. (A simple android application and screenshots of the setup can be found HERE; by the author of openpipeflow.org.) The lines are the time-trace of the lower pendulum, i.e. the state of the system has been projected onto (x,y)=(position of lower pendulum).

As the state of a system changes in time, its 'state-vector' traces out a trajectory. If the state returns to a state that has been seen before, then it traces out a closed 'periodic orbit'.

Observe that the longer orbit (blue) in the example can be considered to be constructed from 'shadowing' of the two simpler orbits. To understand a lot about the dynamics it is sufficient to find the short periodic orbits. These we might call our 'alphabet', out of which infinitely many 'words', i.e. longer orbits, may be constructed.

An excellent (graduate level) free text on periodic orbits can be found at chaosbook.org.

### Periodic orbits in pipe flow

Here, by 'pattern' we mean the speed and direction of flow at each point in space. By listing the velocity at every point on a grid we form a state-vector, **a**=(a1,a2,a3,a4,...). As the grid could be refined indefinitely, the dimension (length) of **a** is formally infinite. In a dissipative system, however, the dynamics typically lives on a space of much smaller dimension, e.g. only a few dozen (unrealistic configurations are not visited by the system). To visualise this space, it is usual to project onto a more meaningful vector, e.g. (x,y)=(energy,dissipation).

The following video shows a selection of periodic orbits in pipe flow, visualised in terms of their input (I), dissipation (D) and kinetic energy (E), relative to their laminar (non-turbulent) values:

The setup for the previous video was pipe flow with flow rate measured by Re=DU/nu=2500 (D=diameter, U=mean axial speed, nu=kinematic viscosity). The next video shows flow in the lab frame. Regions of flow slower than the mean flow are indicated in blue, called 'streaks'. Rotating 'vortex structures' are indicated in yellow. To simplify analysis a 4-fold rotational symmetry has been imposed. This does not significantly affect statistical properties of the flow, e.g. the turbulent friction factor.

When viewed in a moving frame it is possible to see recurring patterns, i.e. periodic orbits (next video). The speed at which the frame moves, however, is different for every periodic orbit. To determine this automatically we use the Method of slices.

Periodic orbits exist that encompass the broad range of observed flow patterns. The following video shows an example of a periodic orbit that is representative a spatially localised patch of turbulence: