Abstract
In the theory of differential inclusions of the form where Φ (q, t) is, for every q and t, a given non-empty convex set in the event space { q, t), the set of points of absolutey continuous integral curves q = q (t), t ≥ t’, of (1) originating from the point {q’, t’) is known as the integral funnel with vertex {q’, t’) for the differential inclusion (1). If integral curves are considered on a time segment (t’, t1), one can speak of a segment of the integral funnel. A segment of the integral funnel, with vertex {q’, t’) for the differential inclusion (1) will be denoted by V (q’, t’, t1). We shall examine the case where the segment V (q’, t’, t1) has a “rigid” lateral boundary in the form of a conoid with vertex {q’, t’).
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This function was first investigated in inclusion with Pontryagin’s maximum principle [88]. This was earlier noted in [110]
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© 1991 Springer Science+Business Media Dordrecht
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Butkovskiy, A.G. (1991). The Boundary of an Integral Funnel of a Differential Inclusion. In: Phase Portraits of Control Dynamical Systems. Mathematics and Its Applications (Soviet Series) , vol 63. Springer, Dordrecht. https://doi.org/10.1007/978-94-011-3258-9_11
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DOI: https://doi.org/10.1007/978-94-011-3258-9_11
Publisher Name: Springer, Dordrecht
Print ISBN: 978-94-010-5437-9
Online ISBN: 978-94-011-3258-9
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