Abstract

Under some conditions, an asymptotic solution containing boundary functions was constructed in a paper by Vasil’eva and Butuzov (Differ. Uravn. 1970, 6(4), 650–664 (in Russian); English transl.: Differential Equations 1971, 6, 499–510) for an initial value problem for weakly non-linear differential equations with a small parameter standing before the derivative, in the case of a singular matrix A ( t ) standing in front of the unknown function. In the present paper, the orthogonal projectors onto k e r A ( t ) and k e r A ( t ) ′ (the prime denotes the transposition) are used for asymptotics construction. This approach essentially simplifies understanding of the algorithm of asymptotics construction.

Highlights

  • IntroductionThe bibliography of publications devoted to singularly perturbed problems is very extensive

  • The bibliography of publications devoted to singularly perturbed problems is very extensive.Most of them deal with problems in which a degenerate equation, following from the original one where a small parameter is equal to zero, is resolvable with respect to a fast component of an unknown variable

  • It allows us to represent the algorithm of the boundary functions method for constructing an asymptotic solution of initial-value singularly perturbed problems in the critical case more clearly than in [4]

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Summary

Introduction

The bibliography of publications devoted to singularly perturbed problems is very extensive. An asymptotic solution containing boundary functions for the initial value problem of the weakly non-linear differential equation in a real m-dimensional space X:. It allows us to represent the algorithm of the boundary functions method for constructing an asymptotic solution of initial-value singularly perturbed problems in the critical case more clearly than in [4]. Note that the projector approach has been used in [10] for constructing the zero-order asymptotic solution for a singularly perturbed linear-quadratic control problem in the critical case. We introduce orthogonal projectors of the space X onto kerA(t) and kerA(t)0 Based on these projectors, the algorithm of constructing the zero-order asymptotic approximation of a solution of problem (1)-(2).

Problem Decomposition
Space Decomposition
Zero-Order Asymptotic Solution
Higher-Order Asymptotic Solutions
Illustrative Example
Conclusions
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