2015
DOI: 10.1007/s11071-015-2015-3
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The solution structure of the Düffing oscillator’s transient response and general solution

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Cited by 10 publications
(2 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%
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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%
“…However, when implementing abovementioned homotopy methods, there can be infinitely possible auxiliary linear operators that satisfy the three basic rules for a given nonlinear equation and a certain set of base functions, but yet there are no mathematical theorems which can guide us to choose a proper linear operator L that can guarantee a convergent and efficient homotopy. 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.…”
Section:   Aq and  mentioning
confidence: 99%