2013
DOI: 10.1007/s10013-013-0048-9
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Higher-Order Variational Problems of Herglotz Type

Abstract: We obtain a generalized Euler-Lagrange differential equation and transversality optimality conditions for Herglotz-type higher-order variational problems. Illustrative examples of the new results are given.

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Cited by 29 publications
(32 citation statements)
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“…As it can be easily checked, this corresponds exactly to the Euler-Lagrange equation for the second-order Herglotz problem in Euclidean spaces studied in [34].…”
mentioning
confidence: 57%
“…As it can be easily checked, this corresponds exactly to the Euler-Lagrange equation for the second-order Herglotz problem in Euclidean spaces studied in [34].…”
mentioning
confidence: 57%
“…As an application, a fractional mechanical system is analyzed with a fractionally generalized velocity that reproduces, for α = 1, the standard Lagrangian of a harmonic oscillator with exponential damping, which also contains the non-damped conservative oscillator. The research here initiated can now be enriched in different directions, by trying to bring to the fractional setting the recent results [28,29,30,31,32] of Santos et al on Herglotz variational problems.…”
Section: Discussionmentioning
confidence: 99%
“…The readers interested in the discrete fractional calculus of variations are refereed to the pioneer work of Bastos et al [8,9]. Here we are interested in the generalized continuous calculus of variations introduced by Herglotz. The generalized variational principle firstly proposed by Gustav Herglotz in 1930 [14] gives a variational principle description of non-conservative systems even when the Lagrangian is autonomous [28,30]. It is essentially based on the following problem: find the trajectories x(t), satisfying given boundary conditions, that extremize (minimize or maximize) the terminal value z(b) of the functional z that satisfies the differential equatioṅ…”
Section: Introductionmentioning
confidence: 99%
“…It consists in the determination of trajectories x(·) and corresponding trajectories z(·) that extremize (maximize or minimize) the value z(b), where L ∈ C 1 ([a, b] × R 2n × R; R). While in [3,4,6] the admissible functions are x(·) ∈ C 2 ([a, b]; R n ) and z(·) ∈ C 1 ([a, b]; R), here we consider (P H ) in the wider class of functions x(·) ∈ P C 1 ([a, b]; R n ) and z(·) ∈ P C 1 ([a, b]; R).…”
Section: (P H )mentioning
confidence: 99%
“…Note that the classical problem of the calculus of variations (1) is a particular case of problem (P ) with φ(x) ≡ 0, g(t, x, u) = u and Ω = R n . In this work we show how the results on Herglotz's problem of the calculus of variations (P H ) obtained in [2,6] can be generalized by using the theory of optimal control. The main idea is simple and consists in rewriting the generalized variational problem of Herglotz (P H ) as a standard optimal control problem (P ), and then to apply available results of optimal control theory.…”
Section: (P H )mentioning
confidence: 99%