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Oscillations, Waves, and Interactions - GWDG

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422 U. Parlitz<br />

current state future state<br />

similar states in the past<br />

whose temporal evolution<br />

is known<br />

?<br />

flow<br />

Figure 12. Local modelling using nearest neighbours in (reconstructed) state space.<br />

known) are some neighbouring (reconstructed) states of this reference state that occurred<br />

(in the given time series) in the past such that their evolution over a period of<br />

time T is already known (as illustrated in Fig. 12). If the dynamical flow in (reconstructed)<br />

state space is continuous then the future values of the neighbouring states<br />

provide good approximations of the future evolution of the reference state. This is<br />

the main idea of the local approach <strong>and</strong> there are several options for further improving<br />

its performance [54]. Local modelling can also be applied to complex extendend<br />

system if a suitable state space reconstruction method is used [55].<br />

An alternative to local modelling are global models, for example given as a superposition<br />

of nonlinear basis functions. Such models have been employed to describe<br />

not only the dynamics of a given system but also its parameter dependence [56]. If<br />

models with good generalisation capabilities are required (i. e., models with good<br />

performance on data not seen during the learning process) it is often advantageous<br />

to use not a single type of model but an ensemble of different models. Averaging<br />

their individual forecasts provides in most cases better results (on average) than any<br />

single model [56,57]. A Matlab T M toolbox ENTOOL for such ensemble modelling<br />

was developed by former DPI students Christian Merkwirth <strong>and</strong> Jörg Wichard. 7<br />

5 Synchronisation of chaotic dynamics<br />

Synchronisation of periodic signals is a well-known phenomenon in physics, engineering<br />

<strong>and</strong> many other scientific disciplines. It was first investigated in 1665 by<br />

Christiaan Huygens who observed that two pendulum clocks hanging at the same<br />

beam of his room oscillated in exact synchrony [58,59]. Huygens made experiments<br />

with his clocks <strong>and</strong> found that the synchronisation originates from invisible vibrations<br />

of the beam enabling some interaction between both oscillators. He reported<br />

his findings on the “sympathy of two clocks” (as he called it) at the Royal Society<br />

of London but it took more than 200 years before research on synchronisation was<br />

continued. J. W. Strutt (Lord Rayleigh) described in the middle of the 19th century<br />

that two (similar) organ pipes sound unisono if placed close together so that they<br />

can interact acoustically [60].<br />

7 It is available at http://zti.if.uj.edu.pl/~merkwirth/entool.htm.

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