1999
DOI: 10.1103/physreve.59.5266
|View full text |Cite
|
Sign up to set email alerts
|

Stabilization of unstable steady states and periodic orbits in an electrochemical system using delayed-feedback control

Abstract: We report numerical and experimental results indicating successful stabilization of unstable steady states and periodic orbits in an electrochemical system. Applying a continuous delayed-feedback technique not only periodic and chaotic oscillations are suppressed via stabilization of steady-state solutions but also the chaotic dynamics can be converted to periodic behavior. In all cases the feedback perturbation vanishes as a target state is attained.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

0
64
0

Year Published

2003
2003
2013
2013

Publication Types

Select...
6
4

Relationship

0
10

Authors

Journals

citations
Cited by 105 publications
(64 citation statements)
references
References 22 publications
0
64
0
Order By: Relevance
“…DFC has been successfully applied to many systems, including the stabilization of coherent modes of laser [5,6]; cardiac systems, [7,8], controlling friction, [9]; chaotic electronic oscillators, [10,11]; chemical systems, [12]. To overcome the limitations of DFC, several modifications have been proposed, [13][14][15][16][17].…”
Section: Introductionmentioning
confidence: 99%
“…DFC has been successfully applied to many systems, including the stabilization of coherent modes of laser [5,6]; cardiac systems, [7,8], controlling friction, [9]; chaotic electronic oscillators, [10,11]; chemical systems, [12]. To overcome the limitations of DFC, several modifications have been proposed, [13][14][15][16][17].…”
Section: Introductionmentioning
confidence: 99%
“…Although time-delayed feedback control has been widely used with great success in real world problems in physics, chemistry, biology, and medicine, e.g. [6][7][8][9][10][11][12][13][14][15][16][17][18][19], a severe limitation used to be imposed by the common belief that certain orbits cannot be stabilized for any strength of the control force. In fact, it had been contended that periodic orbits with an odd number of real Floquet multipliers greater than unity cannot be stabilized by the Pyragas method [20][21][22][23][24][25], even if the simple scheme (2.1) is extended by multiple delays in form of an infinite series [26].…”
Section: Z(t) = F (λ Z(t)) + B[z(t − τ) − Z(t)]mentioning
confidence: 99%
“…The anodic voltage for this set of experiments was modulated as V Z V 0 C DxC gðI ðtÞKI ðtKtÞÞ, where gðI ðtÞKI ðtKtÞÞ was the feedback term intended to enhance the regularity of the spike trains. The control amplitude g and the delay time t were determined as follows (Parmananda et al 1999;Escalera Santos et al 2006). Using the time series provoked by the noise amplitude in figure 4b, a return map (not shown) was constructed by plotting successive interspike intervals (t pC1 versus t p ).…”
Section: Coherence Resonance Controlmentioning
confidence: 99%