Abstract

The adaptive approach of strongly non-linear fast-changing signals identification is discussed. The approach is devised by adaptive sampling based on chaotic mapping “in yourself” of a signal. Presented sampling way may be utilized online in the automatic control of chemical reactor (throughout identification of concentrations and temperature oscillations in real-time), in medicine (throughout identification of ECG and EEG signals in real-time), etc. In this paper, we presented it to identify the Weierstrass function and ECG signal.

Highlights

  • One of fundamental problems in signals analyses and transformation is their identification, most often by means of sampling

  • The determination of the boundary frequency is not always possible in practice, especially in the case of fast-changing signals. Under such circumstances sampling should be performed at uneven time intervals, for example: by adaptive sampling, in which the actual sampling moment depends on the previous sample value

  • The scope of this paper is the adaptive sampling approach that is much easier than the so far described approaches. It is based on uneven adaptive sampling with the use of the chaotic representation of the tested signal

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Summary

Introduction

One of fundamental problems in signals analyses and transformation is their identification, most often by means of sampling. The determination of the boundary frequency is not always possible in practice, especially in the case of fast-changing signals. Under such circumstances sampling should be performed at uneven time intervals, for example: by adaptive sampling, in which the actual sampling moment depends on the previous sample value. The scope of this paper is the adaptive sampling approach that is much easier than the so far described approaches. It is based on uneven adaptive sampling with the use of the chaotic representation of the tested signal. Notations: a, b – Weierstrass function parameters, E – information entropy, N – number of samples, observations horizon, p – probability, t – time, λ – Lyapunov’s exponent, w(t) – function generating nonlinear oscillations

Sampling method
Concluding remarks
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