Abstract
We study the applicability of the standard spline collocation method, on a uniform grid, to linear Volterra integral equations of the second kind with the so-called cordial operators; these operators are noncompact and the applicability of the collocation method becomes crucial in the convergence analysis. In particular, piecewise constant, piecewise linear and piecewise quadratic collocation methods are applicable under wide, quite acceptable conditions. For higher order spline collocation, it is more complicated to carry out an analytical study of the applicability of the method; however, a numerical check is rather simple and this is illustrated by some numerical examples.
Highlights
IntroductionIn the present article we study the applicability of spline collocation methods to the Volterra integral equation t μu(t) = t−1φ(t−1s)u(s) ds + f (t), 0 ≤ t ≤ T,
In the present article we study the applicability of spline collocation methods to the Volterra integral equation t μu(t) = t−1φ(t−1s)u(s) ds + f (t), 0 ≤ t ≤ T, (1.1)where φ ∈ L1(0, 1) is the core of the Volterra integral operator t (Vφu)(t) = t−1φ(t−1s)u(s) ds, 0 ≤ t ≤ T.T
We study the applicability of the standard spline collocation method, on a uniform grid, to linear Volterra integral equations of the second kind with the so-called cordial operators; these operators are noncompact and the applicability of the collocation method becomes crucial in the convergence analysis
Summary
In the present article we study the applicability of spline collocation methods to the Volterra integral equation t μu(t) = t−1φ(t−1s)u(s) ds + f (t), 0 ≤ t ≤ T,. Since the applicability and convergence conditions of spline collocation methods for equations (1.1) and (1.4), and even for a class of related nonlinear equations, are the same in their essence [12, 13], we confine ourselves to the case of the model equation (1.1). We say that the collocation method (1.5) is applicable to equation (1.1) if the homogeneous equation μuN = PN VφuN has in SNm[0, T ] only the trivial solution uN = 0, that is, if there exist the inverses to the m-dimensional operators μI − ΠN,iVφ : SN,i → SN,i, i = 0, 1, .
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