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On-line Access: 2024-08-27

Received: 2023-10-17

Revision Accepted: 2024-05-08

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 ORCID:

Cem Civelek

https://orcid.org/0000-0003-0017-8661

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Frontiers of Information Technology & Electronic Engineering  2020 Vol.21 No.4 P.629-634

http://doi.org/10.1631/FITEE.1900014


Construction of a new Lyapunov function for a dissipative gyroscopic system using the residual energy function


Author(s):  Cem Civelek, Özge Cihanbeğendi

Affiliation(s):  Faculty of Engineering, Department of Electrical and Electronics Engineering, Ege University, Bornova-İzmir 35100, Turkey; more

Corresponding email(s):   cem.civelek@ege.edu.tr, ozge.sahin@deu.edu.tr

Key Words:  Lyapunov function, Residual energy function, Stability of dissipative gyroscopic system


Cem Civelek, Özge Cihanbeğendi. Construction of a new Lyapunov function for a dissipative gyroscopic system using the residual energy function[J]. Frontiers of Information Technology & Electronic Engineering, 2020, 21(4): 629-634.

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Abstract: 
In a dissipative gyroscopic system with four degrees of freedom and tensorial variables in contravariant (right upper index) and covariant (right lower index) forms, a Lagrangian-dissipative model, i.e., {L, D}-model, is obtained using second-order linear differential equations. The generalized elements are determined using the {L, D}-model of the system. When the prerequisite of a Legendre transform is fulfilled, the Hamiltonian is found. The Lyapunov function is obtained as a residual energy function (REF). The REF consists of the sum of Hamiltonian and losses or dissipative energies (which are negative), and can be used for stability by Lyapunov’s second method. Stability conditions are mathematically proven.

耗散陀螺系统的李雅普诺夫函数构造:剩余能量函数方法


Cem CİVELEK1, Özge CİHANBEĞENDİ2
1埃格大学电气与电子工程系工程学部,土耳其伊兹密尔博尔诺瓦,35100
2度库兹•埃路尔大学电气与电子工程系工程学部,土耳其伊兹密尔布卡,35160

摘要:在自由度为4、张量有逆变(右上标)和协变(右下标)形式的耗散陀螺系统中,使用二阶线性微分方程建立拉格朗日耗散模型,即{L, D}模型。通过系统的{L, D}模型确定广义元素。满足勒让德变换先决条件时,可得哈密顿量。剩余能量函数(REF)由哈密顿量及损耗或耗散能量(为负)之和组成,将其作为李雅普诺夫函数,可通过李雅普诺夫第二方法作稳定性分析,并从数学上推导出稳定性条件。

关键词:李雅普诺夫函数;剩余能量函数;耗散陀螺系统稳定性

Darkslateblue:Affiliate; Royal Blue:Author; Turquoise:Article

Reference

[1]Ao P, 2004. Potential in stochastic differential equations: novel construction. J Phys A, 37(3):L25-L30.

[2]Arnold VI, 1989. Mathematical methods of classical mechanics (2nd). Graduate Texts in Mathematics. Springer-Verlag, New York, USA.

[3]Barbashin EA, Krasovsky NN, 1952. On the stability of motion as a whole. Doklady Akademii Nauk SSSR, 86(3):453-546 (in Russian).

[4]Chen J, Guo YX, Mei FX, 2018. New methods to find solutions and analyze stability of equilibrium of nonholonomic mechanical systems. Acta Mech Sin, 34(6):1136- 1144.

[5]Chen LQ, Zu JW, Wu J, 2004. Principal resonance in transverse nonlinear parametric vibration of an axially accelerating viscoelastic string. Acta Mech Sin, 20(3):307-316.

[6]Civelek C, 2018. Stability analysis of engineering/physical dynamic systems using residual energy function. Arch Contr Sci, 28(2):201-222.

[7]Civelek C, Diemar U, 2003. Stability Analysis Using Energy Functions. Internationales Wissenschaftliches Koloquium, Technische Universität Ilmenau, Ilmenau (in German).

[8]Hahn W, 1967. Stability of Motion. Springer-Verlag, Berlin, Heidelberg, Germany.

[9]Heil M, Kitzka F, 1984. Grundkurs Theoretische Mechanik. Springer, Wiesbaden GmbH, Wiesbaden, Germany (in German).

[10]Huang ZL, Zhu WQ, 2000. Lyapunov exponent and almost sure asymptotic stability of quasi-linear gyroscopic systems. Int J Nonl Mech, 35(4):645-655.

[11]Krasovskii NN, 1959. Problems of the Theory of Stability of Motion. Stanford University Press, California, USA.

[12]Kwon C, Ao P, Thouless DJ, 2005. Structure of stochastic dynamics near fixed points. PNAS, 102(37):13029-13033.

[13]Lasalle JP, 1960. Some extensions of Liapunov’s second method. IRE Trans Circ Theory, 7(4):520-527.

[14]Lyapunov AM, 1992. The general problem of the stability of motion. Int J Contr, 55(3):531-534.

[15]Ma YA, Tan QJ, Yuan RS, et al., 2014. Potential function in a continuous dissipative chaotic system: decomposition scheme and role of strange attractor. Int J Bifurc Chaos, 24(2):1450015.

[16]Marino R, Nicosia S, 1983. Hamiltonian-type Lyapunov functions. IEEE Trans Autom Contr, 28(11):1055-1057.

[17]Maschke BMJ, Ortega R, van der Schaft AJ, 2000. Energy- based Lyapunov functions for forced Hamiltonian systems with dissipation. IEEE Trans Autom Contr, 45(8): 1498-1502.

[18]McLachlan RI, Quispel GRW, Robidoux N, 1998. Unified approach to Hamiltonian systems, Poisson systems, gradient systems, and systems with Lyapunov functions or first ıntegrals. Phys Rev Lett, 81(12):2399-2403.

[19]Rouche N, Habets P, Laloy M, 1977. Stability Theory by Liapunov’s Direct Method. Springer-Verlag, New York, USA.

[20]Susse R, Civelek C, 2003. Analysis of engineering systems by means of Lagrange and Hamilton formalisms depending on contravariant, covariant tensorial variables. Forsch Ingen, 68(1):66-74.

[21]Süsse R, Civelek C, 2013. Analysis of coupled dissipative dynamic systems of engineering using extended Hamiltonian H for classical and nonconservative Hamiltonian H*n for higher order Lagrangian systems. Forsch Ingen, 77(1-2):1-11.

[22]Xu W, Yuan B, Ao P, 2011. Construction of Lyapunov function for dissipative gyroscopic system. Chin Phys Lett, 28(5):050201.

[23]Yin L, Ao P, 2006. Existence and construction of dynamical potential in nonequilibrium processes without detailed balance. J Phys A, 39(27):8593-8601.

[24]Ying ZG, Zhu WQ, 2000. Exact stationary solutions of stochastically excited and dissipated gyroscopic systems. Int J Nonl Mech, 35(5):837-848.

[25]Yoshizawa T, 1966. Stability Theory by Liapunov’s Second Method. Mathematical Society of Japan, Tokio, Japan.

[26]Yuan RS, Wang XN, Ma YA, et al., 2013. Exploring a noisy van der Pol type oscillator with a stochastic approach. Phys Rev E, 87(6):062109.

[27]Yuan RS, Ma YA, Yuan B, et al., 2014. Lyapunov function as potential function: a dynamical equivalence. Chin Phys B, 23(1):010505.

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