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Why Instantaneous Values of the “Covariant” Lyapunov Exponents Depend upon the Chosen State-Space Scale

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We explore a simple example of a chaotic thermostated harmonic-oscillator system which exhibits qualitatively different local Lyapunov exponents for simple scale-model constant-volume transformations of its coordinate q and momentum p: {q, p} ! {(Q/s), (sP)}. The time-dependent thermostat variable ζ(t) is unchanged by such scaling. The original (qpζ) motion and the scale-model (QPζ) version of the motion are physically identical. But both the local Gram-Schmidt Lyapunov exponents and the related local “covariant” exponents change with the change of scale. Thus this model furnishes a clearcut chaotic time-reversible example showing how and why both the local Lyapunov exponents and covariant exponents vary with the scale factor s.
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  • Ruby Valley Research Institute Highway Contract 60, Box 601 Ruby Valley, Nevada 89833
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  • Ruby Valley Research Institute Highway Contract 60, Box 601 Ruby Valley, Nevada 89833
Bibliografia
  • [1] H. Bosetti, H.A. Posch, Ch. Dellago and Wm.G. Hoover, Time-Reversal Symmetry and Covariant Lyapunov Vectors for Simple Particle Models in and out of Thermal Equilibrium, arXiv:1004.4473, Version 1 (2010); Physical Review E 82, 046218 (2010).
  • [2] H.A. Posch, Symmetry Properties of Orthogonal and Covariant Lyapunov Vectors and Their Exponents, arXiv:1107.4032 (2012); Journal of Physics A: Mathematical and Theoretical 46, 254006 (2013).
  • [3] H-L. Yang and G. Radons, Comparison between Covariant and Orthogonal Lyapunov Vectors, Physical Review E 82, 046204 (2010).
  • [4] F. Ginelli, P. Poggi, A. Turchi, H. Chaté, R. Livi, and A. Politi, Characterizing Dynamics with Covariant Lyapunov Vectors Physical Review Letters 99, 130601 (2007).
  • [5] M. Romero-Bastida, D. Pazó, J.M. López, and M.A. Rodríguez, Structure of Characteristic Lyapunov Vectors in Anharmonic Hamiltonian Lattices, Physical Review E 82, 036205 (2010).
  • [6] C.L. Wolfe and R.M. Samelson. An Efficient Method for Recovering Lyapunov Vectors from Singular Vectors, Tellus 59A, 355-366 (2007).
  • [7] W.G. Hoover and H.A. Posch, Direct Measurement of Lyapunov Exponents, Physics Letters A 113, 82-84 (1985).
  • [8] Wm.G. Hoover and C.G. Hoover, Local Gram-Schmidt and Covariant Lyapunov Vectors and Exponents for Three Harmonic Oscillator Problems, Communications in Nonlinear Science and Numerical Simulation 17, 1043-1054 (2012).
  • [9] Wm.G. Hoover, C.G. Hoover, and H.A. Posch, Lyapunov Instability of Pendulums, Chains, and Strings, Physical Review A 41, 2999-3004 (1990).
  • [10] H.A. Posch and Wm.G. Hoover, Time-Reversible Dissipative Attractors in Three and Four Phase-Space Dimensions, Physical Review E 55, 6803-6810 (1997).
  • [11] Wm.G. Hoover, Canonical Dynamics: Equilibrium Phase-Space Distributions, Physical Review A 31, 1695-97 (1985).
  • [12] H.A. Posch, Wm.G. Hoover, and F.J. Vesely, Canonical Dynamics of the Nosé Oscillator: Stability, Order, and Chaos, Physical Review A 33, 4253-4265 (1986).
  • [13] Wm.G. Hoover, Remark on ‘Some Simple Chaotic Flows’, Physical Review E 51, 759-760 (1995).
  • [14] J.C. Sprott, Some Simple Chaotic Flows, Physical Review E 50, R647-R650 (1994).
  • [15] Wm.G. Hoover and C.G. Hoover, Time-Symmetry Breaking in Hamiltonian Mechanics, arXiv 1302.2533 (2013); Computational Methods in Science and Technology 19, 77-87 (2013).
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Bibliografia
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bwmeta1.element.baztech-eb49e2f4-fcb3-4ed4-9023-26e1a98aa277
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