Abstract
FOR THE solution by a difference method of the problem on eigenvalues Lu + λru = 0, u(0) = u ( i) = 0, Lu = ( u′ p )′ − qu , 0 < c i ⩽ p( x) ⩽ c 2, 0 ⩽ q( x) ⩽ c 3, 0 < c 4 ⩽ r( x) ⩽ c 5, on the assumption that the coefficients p( x), q( x) and r( x) are sufficiently smooth, the asymptotics of the eigenvalues, calculated by schemes of the 2nd and 4th orders of accuracy, are obtained in [1]. In [2] taking into account certain terms of the asymptotic expansion of the error of the eigenvalues, the evaluation Δλ was found for the solution, by the simplest scheme of the second order of accuracy, of the problem u′' + λru = 0, u(0) = u(1) = 0, r( x) ϵ C (4) (0,1). For the boundary value problem Lu = − f, u(0) = u 0, u(1) = u 1 in [3] an exact scheme is put forward and also schemes of any order of accuracy obtained from it, which are constructed on a non-uniform network in the class of piecewise continuous functions p, q, and r. These schemes are used in [4] in the construction of schemes of a higher order of accuracy for problem (1). In the present paper asymptotic formulae are given for the error of the eigenvalues which appear in the schemes of [4]. The peculiarity of the given formulae lies in the fact that they are obtained only on the assumption of piecewise continuity of the original data p( x), q( x) and r( x).
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
More From: USSR Computational Mathematics and Mathematical Physics
Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.