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Phase-lag analysis of explicit Nyström methods fory″=f(x,y)

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Abstract

We examine phase-lag (frequency distortion) of the two-parameter familyM 41, α3) of fourth order explicit Nyström methods of [1] by applying these to the test equation:y″+λ 2 y=0, λ>0. While the methodM 4(1/6, 5/6) possessing the largest interval of periodicity of size 3.46 has a phase-lag of (1/4320)H (H 4=λh, h is the step-size), we show that there exist two fourth order methods ofM 41, α3) for which the phase-lag is minimal and of size (1/40320)H 6; interestingly, both methods also possess a sizable interval of periodicity of length 2.75 each.

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References

  1. M. M. Chawla and S. R. Sharma,Intervals of periodicity and absolute stability of explicit Nyström methods for y″=f(x,y), BIT 21 (1981), 455–464.

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  2. L. Brusa and L. Nigro,A one-step method for direct integration of structural dynamic equations, Internat. J. Numer. Methods Engrg. 15 (1980), 685–699.

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Chawla, M.M., Rao, P.S. Phase-lag analysis of explicit Nyström methods fory″=f(x,y) . BIT 26, 63–70 (1986). https://doi.org/10.1007/BF01939362

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  • DOI: https://doi.org/10.1007/BF01939362

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