2019
DOI: 10.1016/j.asej.2018.08.007
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Generalization of the modified Lindstedt-Poincare method for solving some strong nonlinear oscillators

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Cited by 20 publications
(44 citation statements)
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“…5.2 that the values of these coefficients are opposite in sign when 19 32 < k. But all are positive when k ≤ 19 32 and δ 2 vanishes when k = 19 32 . Thus for k = 1 and k = 19 32 , we have obtained respectively a 0 ω(k = 1) ω(k = Table 1: Comparison of the approximate frequencies obtained by present method with the numerical and other existing frequencies (Alam et al [14] and Cheung et al [6], k = 1) for the Duffing oscillator (where Er(%) denotes absolute percentage error). Comparing these results, we easily expect that α-series (Eq.…”
Section: Resultsmentioning
confidence: 75%
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“…5.2 that the values of these coefficients are opposite in sign when 19 32 < k. But all are positive when k ≤ 19 32 and δ 2 vanishes when k = 19 32 . Thus for k = 1 and k = 19 32 , we have obtained respectively a 0 ω(k = 1) ω(k = Table 1: Comparison of the approximate frequencies obtained by present method with the numerical and other existing frequencies (Alam et al [14] and Cheung et al [6], k = 1) for the Duffing oscillator (where Er(%) denotes absolute percentage error). Comparing these results, we easily expect that α-series (Eq.…”
Section: Resultsmentioning
confidence: 75%
“…We have introduced k in the first approximate solution and consequently k appear in the second, third and fourth approximations. Choosing a suitable value of k, we can find a series of ω which converge faster than that of obtained by Cheung et al [6] and Alam et al [14].…”
Section: Examplementioning
confidence: 77%
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