An Essential Extension of the Finite-Energy Condition for Extended Runge-Kutta-Nystrom Integrators when Applied to Nonlinear Wave Equations
被引:19
作者:
Mei, Lijie
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机构:
Shangrao Normal Univ, Sch Math & Comp Sci, Shangrao 334001, Peoples R ChinaShangrao Normal Univ, Sch Math & Comp Sci, Shangrao 334001, Peoples R China
Mei, Lijie
[1
]
Liu, Changying
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Nanjing Univ, Dept Math, Nanjing 210093, Jiangsu, Peoples R China
Nanjing Univ, State Key Lab Novel Software Technol, Nanjing 210093, Jiangsu, Peoples R ChinaShangrao Normal Univ, Sch Math & Comp Sci, Shangrao 334001, Peoples R China
Liu, Changying
[2
,3
]
Wu, Xinyuan
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机构:
Qufu Normal Univ, Sch Math Sci, Qufu 273165, Peoples R ChinaShangrao Normal Univ, Sch Math & Comp Sci, Shangrao 334001, Peoples R China
Wu, Xinyuan
[4
]
机构:
[1] Shangrao Normal Univ, Sch Math & Comp Sci, Shangrao 334001, Peoples R China
[2] Nanjing Univ, Dept Math, Nanjing 210093, Jiangsu, Peoples R China
[3] Nanjing Univ, State Key Lab Novel Software Technol, Nanjing 210093, Jiangsu, Peoples R China
[4] Qufu Normal Univ, Sch Math Sci, Qufu 273165, Peoples R China
This paper is devoted to an extension of the finite-energy condition for extended Runge-Kutta-Nystr "om (ERKN) integrators and applications to nonlinear wave equations. We begin with an error analysis for the integrators for multi-frequency highly oscillatory systems y'' + M y = f (y), where M is positive semi-definite, parallel to M parallel to >>parallel to partial derivative f/partial derivative y parallel to, and parallel to M parallel to >> 1. The highly oscillatory system is due to the semi-discretisation of conservative, or dissipative, nonlinear wave equations. The structure of such a matrix M and initial conditions are based on particular spatial discretisations. Similarly to the error analysis for Gaustchi-type methods of order two, where a finite-energy condition bounding amplitudes of high oscillations is satisfied by the solution, a finiteenergy condition for the semi-discretisation of nonlinear wave equations is introduced and analysed. These ensure that the error bound of ERKN methods is independent of parallel to M parallel to. Since stepsizes are not restricted by frequencies of M, large stepsizes can be employed by our ERKN integrators of arbitrary high order. Numerical experiments provided in this paper have demonstrated that our results are truly promising, and consistent with our analysis and prediction.