共查询到20条相似文献,搜索用时 15 毫秒
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《Physica D: Nonlinear Phenomena》1988,31(2):190-211
A physical system is considered consisting of a rigid frame which is free to rotate about a vertical axis and to which is attached a planar simple pendulum. This system has “one and a half” degrees of freedom due to the fact that the frame and pendulum may freely rotate about the vertical axis, i.e., conservation of angular momentum holds for the “ideal”, or unperturbed, system. Using a Hamiltonian formulation we reduce the unperturbed equations of motion to a conservative planar system in which the constant angular momentum plays the role of a parameter. This system is shown to possess one or two sets of homoclinic motions depending on the level of the angular momentum. When this system is perturbed by external excitations and dissipative forces these homoclinic motions can break into homoclinic tangles providing the conditions for chaotic motions of the horseshoe type to exist. The criteria for this to occur can be formulated using a variation of Melnikov's method developed for slowly varying oscillators [1, 2]. For the present problem, the angular momentum becomes a slowly varying parameter upon addition of the disturbances. These ideas are used to rigorously prove the existence of chaotic motions for this system and to compute, to first order, global bifurcation parameter conditions. Since two types of homoclinic motions can occur, two different chaotic modes of motion can result and physical interpretations of these motions are given. In addition, a limiting case is considered in which the system becomes a single degree of freedom oscillator with parametric excitation. 相似文献
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V. V. Vecheslavov 《Journal of Experimental and Theoretical Physics》2004,98(2):352-358
An analysis of the stochastic layer in a driven pendulum is extended to the case when the separatrix map contains both single-and double-frequency harmonics. Resonance invariants of the first three orders are found for the double-frequency harmonic. Combined with the previously known single-frequency invariants, they can be used to obtain further information about the layer, in particular, to examine the neighborhoods of zeros of Melnikov integrals. 相似文献
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《Physica D: Nonlinear Phenomena》1986,19(2):238-254
Rational pole-solutions of a perturbed KdV equation, describing nonlinear ion-acoustic plasma waves, become chaotic in time, when a small perturbation is periodically driven. A McGehee transformation blows up a degenerate stationary point at infinity and the Smale-Birkhoff Homoclinic. Theorem adapted to submanifolds in phase permits the use of the Melnikov method, with pole-solutions being homoclinic orbits. 相似文献
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We analyse the use of parametric and quasiperiodic modulations in suppressing horseshoe structure in the phase plane of perturbed
pendulum systems. Taking the Froude pendulum as a typical system, four different modulation mechanisms are studied by deriving
analytic expressions for the window of the strength of modulation giving suppression in each case. A comparison of the four
cases from the point of view of flexibility and efficiency is also given. 相似文献
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V. V. Vecheslavov 《Journal of Experimental and Theoretical Physics》2004,99(3):663-668
An analysis of the stochastic layer in a pendulum driven by an asymmetric high-frequency perturbation of fairly general form is continued. Analytical expressions are found for the amplitudes of secondary harmonics, and their contributions to the amplitude of the separatrix map responsible for onset of dynamical chaos are evaluated. Additional evidence is presented of the previously established fact that the secondary harmonics completely determine the stochasticl-ayer width when the primary frequencies lie in certain intervals. The mechanism of the onset of chaos in the vicinity of zeros of Melnikov integrals is shown to be substantially different as compared to the previously analyzed case of symmetric perturbation. 相似文献
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L. A. Prokudina 《Journal of Experimental and Theoretical Physics》2014,118(3):480-488
A mathematical model is presented for the state of a free surface of a thin fluid layer (a fluid film) in heat-mass-exchange processes of condensation and evaporation. The wave motion of a fluid film is studied under inhomogeneous surface tension. Nonlinear development of perturbations belonging to a continuous band of wave numbers on the surface of a thin fluid layer is investigated within the framework of a non-linear parabolic equation. It is shown that wave packets with carrier wave lying near the harmonic of maximum increment become self-ordered; as a result, a monochromatic wave is generated on the surface of the fluid film. When a wave packet is generated in the neighborhood of the neutral stability curve, one can observe a phenomenon of directed energy transfer to the waves in the neighborhood of the harmonic of maximum increment. 相似文献
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V. V. Kozlov I. D. Zverkov B. Yu. Zanin A. V. Dovgal V. Ya. Rudyak E. G. Bord D. F. Kranchev 《Thermophysics and Aeromechanics》2006,13(4):507-514
Laminar-turbulent transition in a boundary layer of low-aspect-ratio wing was investigated. Experiments clarifying the flow
structure, its mean and oscillatory characteristics were carried out accompanied by linear stability analysis of the wind
tunnel data on the laminar flow velocity profiles. Theoretical results obtained in a parallel flow approximation are in a
good agreement with the experimental data on disturbances evolution at the initial stage of transition to turbulence.
The study was supported by the Ministry of Education and Science of the Russian Federation (Grant No. RNP 2.1.1.471) and Russian
Foundation for Basic Research (Grant No. 03-01-06145) 相似文献
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The chaotic time oscillations in an incompressible fluid driven into motion by a harmonic time-varying pressure gradient is examined. Special attention is given to centrifugal destabilization of the viscous boundary layer. The basic flow is shown to be linearly unstable. For increasing modulation amplitude, the flow exhibits chaotic oscillations. The energy exchange between subharmonics and superharmonics of the least-stable spanwise wave number is considered. The presence of subharmonic Fourier modes are shown to accelerate the transition to temporally chaotic motion. (c) 1996 American Institute of Physics. 相似文献
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《Superlattices and Microstructures》2005,37(3):185-191
The robustness of limit cycles of nonlinear dynamical systems is investigated by adding a small random velocity field to the famous van der Pol (VDP) equation in its two-dimensional phase plane. Our numerical calculations show that a limit cycle does not change much under a weak random perturbation. Thus it confirms the conjecture that a limit cycle will make only a small deformation under an external perturbation. The idea can be used to understand the ac response of self-sustained oscillations in nonlinear dynamical systems. 相似文献
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《Physics Reports》1988,157(2):63-181
The dynamics of solitons is investigated in media with randomly inhomogeneous and fluctuating parameters. Some exact results of the theory of nonlinear stochastic waves are given. An analysis is made of various approximate approaches, e.g. of the mean field method and the Born approximation. Special attention is paid to the perturbation technique based on the inverse scattering transform and to the construction of the most adequate stochastic perturbation theory for solitons. The described formalism is used to investigate the evolution of nonlinear wave (soliton) parameters, and the statistical characteristics of radiation generated by solitons in fluctuating media are analysed also. The same approach makes it possible to take into account the simultaneous effect of random and regular (e.g., friction) perturbations on the dynamics of solitons. Examples are given of situations arising when one describes nonlinear waves in real physical systems. 相似文献
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A. Yu. Dyachenko Ya. I. Smul’sky V. I. Terekhov N. I. Yarygina 《Thermophysics and Aeromechanics》2015,22(6):677-688
In the present paper, we consider one of the most efficient and simple methods to additionally intensify the exchange processes and heat transfer in the separated flow behind a backward-facing step. The method uses small obstacles installed upstream the step; such obstacle act as turbulators smaller in size than the main obstacle. As the turbulators, solid mini ribs, comb ribbings, and wall-detached mini ribs were used. Intensification of the turbulent mixing process behind the main obstacle occurs due to the introduction of small-obstacle-induced 2D and 3D perturbations into the separated shear layer behind the step. Results of a detailed experimental study of the distributions of pressure and heat transfer for different heights of the small intensifier and its positions with respect to the step are reported. The influence of intensifier shape on the thermal and dynamic characteristics of the flow has been analyzed. The distributions of pressure and heat-transfer coefficients were used to evaluate the effectiveness of the various mini obstacles and the limits of their action on the drag and heat transfer. 相似文献
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The chaotic behaviour and limit cycle behviaiour of the dynamical system is investigated for various potentials V and parameters values α, and . 相似文献
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