2010
DOI: 10.1088/1751-8113/43/17/175205
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A direct approach to the construction of standard and non-standard Lagrangians for dissipative-like dynamical systems with variable coefficients

Abstract: We present a direct approach to the construction of Lagrangians for a large class of one-dimensional dynamical systems with a simple dependence (monomial or polynomial) on the velocity. We rederive and generalize some recent results and find Lagrangian formulations which seem to be new. Some of the considered systems (e.g., motions with the friction proportional to the velocity and to the square of the velocity) admit infinite families of different Lagrangian formulations.

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Cited by 95 publications
(162 citation statements)
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References 43 publications
(100 reference statements)
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“…so the discrete curve x obtained by iteration of the contact map satisfies the discrete Herglotz variational principle for L. Note that x need not be a scalar: the Lagrangian L = 1 2 |ẋ| 2 − V (x) − αz yields the analogous multi-component equation. This contrasts many other variational descriptions of the damped harmonic oscillator, which only apply to the scalar case [44,15]. The same comment applies to the following discretization, which we write down for scalar x but can easily be adapted to higher dimensions.…”
Section: Discrete Herglotz Variational Principlementioning
confidence: 93%
“…so the discrete curve x obtained by iteration of the contact map satisfies the discrete Herglotz variational principle for L. Note that x need not be a scalar: the Lagrangian L = 1 2 |ẋ| 2 − V (x) − αz yields the analogous multi-component equation. This contrasts many other variational descriptions of the damped harmonic oscillator, which only apply to the scalar case [44,15]. The same comment applies to the following discretization, which we write down for scalar x but can easily be adapted to higher dimensions.…”
Section: Discrete Herglotz Variational Principlementioning
confidence: 93%
“…After the oscillators considered in Sections 3 and 4, we change gears slightly and consider two classes of variable-coefficients dissipative oscillators that have been treated recently in [6].…”
Section: Dissipative Oscillatorsmentioning
confidence: 99%
“…Section 4 investigates a special case of the generalized anharmonic oscillator given in [7]. Section 5 considers two classes of dissipative dynamical systems with variable coefficients [6]. The Lane-Emden equation [10] is treated in Section 6.…”
Section: Introductionmentioning
confidence: 99%
“…They were introduced by Arnold since 1978 [1], R. A. El-Nabulsi (B) College of Mathematics and Information Science, Neijiang Normal University, Neijiang 641112, Sichuan, China e-mail:nabulsiahmadrami@yahoo.fr but they were ignored for a good period of time due to the lack of their Hamiltonian formalisms. Their roles in the theory of differential equations [2][3][4], dissipative systems [5][6][7][8][9][10][11][12] and theoretical physics [13][14][15][16][17] are well appreciated. Despite the fact that a solid and comprehensive Hamiltonian formulation is missed, NSL are considered to be good candidates to explain dissipative dynamical systems.…”
Section: Introductionmentioning
confidence: 99%