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首页> 外文期刊>International Journal of Mechanical Sciences >Forced vibration of axially moving beam with internal resonance in the supercritical regime
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Forced vibration of axially moving beam with internal resonance in the supercritical regime

机译:超临界方案中具有内部共振的轴向移动光束的强制振动

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Local and global resonances under the condition of 3:1 internal resonance of a super-critically axially moving beam, subjected to a harmonic exciting force, are investigated in the present work. The governing equation is derived from the generalized Hamilton's principle and discreted into a multiple-degrees-of-freedom system by the Galerkin's method. In the super-critical regime, the axially moving beam becomes a bistable system with two symmetrical non-trivial equilibrium configurations. Based on the transformation around one of them, natural frequencies and the condition of internal resonance are obtained. By employing the method of multiple scales, resonances for first-two modes and harmonics under the condition of internal resonance are discussed analytically. Total displacement at the middle of the beam is composed by them and confirmed by direct numerical method. Internal resonance is found to have a big effect on the phase angle of and the amplitude. Coupling ship between the first-two modes is verified to be produced by the cubic nonlinearity and the 3:1 commensurability together. The effect of moving speed acting on the internal resonance is discussed and an energy transmission region is found. Different with the internal resonance in the sub-critical regime, most of the transferred energy is absorbed by the quadratic nonlinearity in the super-critical regime. The critical excitation of the local response is predicted by the analytical method and certified by simulations. The global response for the primary resonance has two stable focal points. However, the global response for the secondary resonance only has one stable focal point for the non-trivial equilibrium configuration is counteracted. (C) 2017 Elsevier Ltd. All rights reserved.
机译:在本作工作中研究了在3:1的条件下的局部和全局共振,其经受谐波激动力的超强轴向移动的梁的内部共振。管理方程源自广义汉密尔顿原则,并通过Galerkin的方法离散到多程度的自由度系统中。在超临界状态下,轴向移动的梁成为具有两个对称的非差距平衡配置的双稳态系统。基于其中一个的变换,获得自然频率和内部共振的条件。通过采用多种尺度的方法,分析地讨论了在内部共振条件下的前两种模式和谐波的共振。光束中间的总位移由它们组成并通过直接数值方法确认。发现内部共振对相位角和振幅具有很大影响。验证了前两种模式之间的耦合船以由立方非线性和3:1在一起产生的。讨论了作用在内部谐振上的移动速度的效果,并找到能量传输区域。与子临界制度中的内部共振不同,大部分转移能量被超临界制度中的二次非线性吸收。通过分析方法预测本地响应的临界激励,并通过模拟认证。初级共振的全局响应有两个稳定的焦点。然而,二次谐振的全局响应仅抵消了非琐静平衡配置的一个稳定的焦点。 (c)2017 Elsevier Ltd.保留所有权利。

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