Original Article
Journal of Low Frequency Noise,
Vibration and Active Control
2021, Vol. 0(0) 1–25
© The Author(s) 2021
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DOI: 10.1177/14613484211026407
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Hybrid rayleigh–van der pol–duffing
oscillator: Stability analysis and controller
Chun-Hui He
1,2
, Dan Tian
3
, Galal M Moatimid
4
,
Hala F Salman
5
and Marwa H Zekry
6
Abstract
The current study examines the hybrid Rayleigh–Van der Pol–Duffing oscillator (HRVD) with a cubic–quintic nonlinear
term and an external excited force. The Poincar´ e–Lindstedt technique is adapted to attain an approximate bounded
solution. A comparison between the approximate solution with the fourth-order Runge–Kutta method (RK4) shows a
good matching. In case of the autonomous system, the linearized stability approach is employed to realize the stability
performance near fixed points. The phase portraits are plotted to visualize the behavior of HRVD around their fixed points.
The multiple scales method, along with a nonlinear integrated positive position feedback (NIPPF) controller, is employed to
minimize the vibrations of the excited force. Optimal conditions of the operation system and frequency response curves
(FRCs) are discussed at different values of the controller and the system parameters. The system is scrutinized numerically
and graphically before and after providing the controller at the primary resonance case. The MATLAB program is employed
to simulate the effectiveness of different parameters and the controller on the system. The calculations showed that NIPPF
is the best controller. The validations of time history and FRC of the analysis as well as the numerical results are satisfied by
making a comparison among them.
Keywords
hybrid Rayleigh–Van der Pol–Duffing oscillator, Poincar´ e–Lindstedt technique, linearized stability, multiple scales method,
nonlinear integral positive position feedback
Introduction
Nonlinear vibration provides an interesting potential example of the mathematical description of the nonlinear behavior of
many phenomena in science, physics, and practical engineering; for example, the N/MEMS system vibrates nonlinearly.
1-7
The nonlinear wave equation of Kundu–Mukherjee–Naskar equation can be finally converted into a Duffing-like equation.
8
Fangzhou oscillator is a generalized Duffing equation (DE) with a singular term.
9-11
The nonlinear vibration systems in a
porous medium can be converted to a fractal modification of the DE.
12-14
The gecko-like vibration plays an important role
in the accurate 3-D printing process.
15
The inherent pull-in instability of MEMS systems can be completely overcome by
the fractal vibration theory.
16-18
The homotopy perturbation method (HPM)
19
and the Hamitonian approach
20
are two main
analytical tools for nonlinear vibration systems. The combination of the Laplace transforms, Lagrange multiplier, fractional
1
Xi’an University of Architecture & Technology, Xi’an, PR China
2
National Engineering Laboratory for Modern Silk, College of Textile and Clothing Engineering, Soochow University, Suzhou, China
3
School of Science, Xi’an University of Architecture and Technology, Xi’an, China
4
Department of Mathematics, Faculty of Education, Ain Shams University, Cairo, Egypt
5
Department of Basic Sciences, Faculty of Computers and Artificial Intelligence, Cairo University, Giza, Egypt
6
Department of Mathematics and Computer Science, Faculty of Sciences, Beni-Suef University, Beni-Suef, Egypt
Corresponding author:
Dan Tian, School of Science, Xi’an University of Architecture and Technology, Xi’an, China.
Email: tiandan@xauat.edu.cn
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