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首页> 外文期刊>International journal of non-linear mechanics >Interaction of free and forced nonlinear normal modes in two-DOF dissipative systems under resonance conditions
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Interaction of free and forced nonlinear normal modes in two-DOF dissipative systems under resonance conditions

机译:共振条件下两自由度耗散系统中自由和强迫非线性法线模式的相互作用

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The resonance dynamics of a dissipative spring-mass and of a dissipative spring-pendulum system is studied. Internal resonance case is considered for the first system; both external resonances and simultaneous external and internal resonance are studied for the second one. Analysis of the systems resonance behavior is made on the base of the concept of nonlinear normal vibration modes (NNMs) by Kauderer and Rosenberg, which is generalized for dissipative systems. The multiple time scales method under resonance conditions is applied. The resulting equations are reduced to a system with respect to the system energy, arctangent of the amplitudes ratio and the difference of phases of required solution in the resonance vicinity. Equilibrium positions of the reduced system correspond to nonlinear normal modes; in energy dissipation case they are quasi-equilibriums. Analysis of the equilibrium states of the reduced system permits to investigate stability of nonlinear normal modes in the resonance vicinity and to describe transfer from unstable vibration mode to stable one. New vibration regimes, which are called transient nonlinear normal modes (TNNMs) are obtained. These regimes take place only for some particular levels of the system energy. In the vicinity of values of time, corresponding to these energy levels, the TTNM attract other system motions. Then, when the energy decreases, the transient modes vanish, and the system motions tend to another nonlinear normal mode, which is stable in the resonance vicinity. The reliability of the obtained analytical results is confirmed by numerical and numerical-analytical simulations.
机译:研究了耗散弹簧质量和耗散弹簧摆系统的共振动力学。对于第一个系统,考虑内部共振情况;第二阶段研究了外部共振以及同时发生的内部和外部共振。系统共振行为的分析是基于Kauderer和Rosenberg的非线性法向振动模式(NNM)的概念进行的,该模型通常用于耗散系统。采用了共振条件下的多时间尺度方法。相对于系统能量,振幅比的反正切以及共振附近所需解的相位差,将所得方程简化为系统。简化系统的平衡位置对应于非线性法线模式。在能量耗散的情况下,它们是准平衡的。通过对简化系统的平衡态进行分析,可以研究共振附近非线性正态模的稳定性,并描述从不稳定振动模态向稳定振动模态的转换。获得了新的振动状态,称为瞬态非线性法线模式(TNNM)。这些机制仅在系统能量的某些特定级别发生。在与这些能量水平相对应的时间值附近,TTNM会吸引其他系统运动。然后,当能量减少时,瞬态模式消失,系统运动趋向于另一个非线性法线模式,该模式在共振附近稳定。数值和数值模拟仿真证实了所获得分析结果的可靠性。

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