2017
DOI: 10.1007/s11075-017-0420-z
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On the limit cycles, period-doubling, and quasi-periodic solutions of the forced Van der Pol-Duffing oscillator

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Cited by 17 publications
(14 citation statements)
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“…To be specific, when solving nonlinear oscillator problems with the HAM, it is straightforward to choose time-related trigonometric functions as base functions to express the steady-state solution [23,24] or exponential and trigonometric functions for transient state [25]. But various single-frequency or multifrequency auxiliary linear operators with or without damping terms can all meet the basic requirements for constructing a homotopy [23][24][25][26][27][28], and there are no universally applicable rules on how to choose the effective ones. Currently, a proper choice on L requires not only sufficient mathematical knowledge, but also extensive experience in applying the HAM, especially for problems with strong and hybrid nonlinearities.…”
Section:   Aq and  mentioning
confidence: 99%
“…To be specific, when solving nonlinear oscillator problems with the HAM, it is straightforward to choose time-related trigonometric functions as base functions to express the steady-state solution [23,24] or exponential and trigonometric functions for transient state [25]. But various single-frequency or multifrequency auxiliary linear operators with or without damping terms can all meet the basic requirements for constructing a homotopy [23][24][25][26][27][28], and there are no universally applicable rules on how to choose the effective ones. Currently, a proper choice on L requires not only sufficient mathematical knowledge, but also extensive experience in applying the HAM, especially for problems with strong and hybrid nonlinearities.…”
Section:   Aq and  mentioning
confidence: 99%
“…The importance of high precision computation in applied mathematics and science need not be overemphasized [5]. The higher precision quantitatively accurate computation of periodic orbits is facilitated in the framework of a novel asymptotic analysis [6][7][8][9], so as to allow significant numerical improvements in the computations of periodic orbits by the conventional asymptotic techniques such as renormalization group method(RGM) [10], multiple scale method (MSM) [1], homotopy analysis method [11,12] etc. As a prototype of strongly nonlinear oscillator, we consider here singularly perturbed Rayleigh Equation (SRLE) [1,4] equation with an external periodic excitation…”
Section: Introductionmentioning
confidence: 99%
“…Existence of slow and fast motions makes traditional analytical techniques ineffective in an efficient estimation of such relaxation oscillations [15,16]. Dynamical systems experiencing the fast-slow motions appear widely in engineering and other applied sciences [12]. The slow-fast periodic motions in such dynamical systems cannot be easily tackled, because such slow-fast periodic motions need many more harmonic terms to get appropriate approximate solutions.…”
Section: Introductionmentioning
confidence: 99%
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