2015
DOI: 10.1002/acs.2564
|View full text |Cite
|
Sign up to set email alerts
|

Sinusoidal disturbance rejection in chaotic planar oscillators

Abstract: The main goal of this paper is to design a compensator able to restore the nominal behavior of a planar system, which is rendered chaotic by an unmeasurable sinusoidal disturbance input. To reach such a goal, some instruments, taken from algebraic geometry, are used to estimate the unmeasurable disturbance from the time derivatives of the output of the system and of the control input.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
2

Citation Types

0
9
0
1

Year Published

2016
2016
2022
2022

Publication Types

Select...
4
2

Relationship

1
5

Authors

Journals

citations
Cited by 16 publications
(10 citation statements)
references
References 31 publications
0
9
0
1
Order By: Relevance
“…g 2, 1 = 2y (3) + y (4) − y (5) , g 2, 2 = 4y (2) − 3y (4) + y (5) , g 2, 3 = 8y (1) + 5y (4) − 3y (5) , g 2, 4 = 16y (0) − 11y (4) + 5y (5) ,…”
Section: ẋ(T) = a X(t) Y(t) =unclassified
See 2 more Smart Citations
“…g 2, 1 = 2y (3) + y (4) − y (5) , g 2, 2 = 4y (2) − 3y (4) + y (5) , g 2, 3 = 8y (1) + 5y (4) − 3y (5) , g 2, 4 = 16y (0) − 11y (4) + 5y (5) ,…”
Section: ẋ(T) = a X(t) Y(t) =unclassified
“…Hence, by considering that y (1) y (2) y (3) y (4) y (5) , y (1) y (2) y (3) y (4) y (5) , and that the matrices on the right-hand side of the expressions above have full rank, by the same reasoning used in the proof of Theorem 1, one has that ⟨g 1, 1 , g 1, 2 , g 2, 1 , g 2, 2 , g 2, 3 , g 2, 4 ⟩ = ⟨y (0) , y (1) , …, y (5) ⟩, ⟨g 1, 3 , g 1, 4 , g 3, 1 , g 3, 2 , g 3, 3 , g 3, 4 ⟩ = ⟨y (0) , y (1) , …, y (5) ⟩ .…”
Section: ẋ(T) = a X(t) Y(t) =mentioning
confidence: 99%
See 1 more Smart Citation
“…In this work, we extend the proposed methodology to the problem of output-disturbance decoupling with internal stability. The problem of decoupling, attenuating or rejecting the effect of perturbation acting over a nonlinear plant is of paramount importance from both practical and methodological points of view [11,12,13,14,15,16,17,18]. As well known, given a general plant disturbance decoupling is related to generating unobservability so to make the output evolutions independent upon the perturbations acting over the dynamics ([19, 20, 21, 22, 23]).…”
Section: Introductionmentioning
confidence: 99%
“…The paper in [8] investigates a control law for a class of chaotic planar oscillators which is able to restore their nominal dynamical behavior(i.e., the non-chaotic one, which is obtained in the absence of a disturbance). In particular, the authors make use of algebraic geometry to express the amplitude and the frequency of the sinusoidal disturbance as functions of the time derivatives of the control input and of the output.…”
Section: Introductionmentioning
confidence: 99%