The analysis of aerolastic airfoil with freeplay stuctural nonlinearity in pitch using Poincare map

来源 :第十二届全国非线性振动暨第九届全国非线性动力学和运动稳定性学术会议 | 被引量 : 0次 | 上传用户:xiexia1987623
下载到本地 , 更方便阅读
声明 : 本文档内容版权归属内容提供方 , 如果您对本文有版权争议 , 可与客服联系进行内容授权或下架
论文部分内容阅读
Investigation the two degree-of-freedom(DOF) wedge aeroelastic airfoil with combined freeplay and cubic nonlinearity in pitch submitted to supersonic and hypersonic flow is significant and critical for designing of the aircraft structural control surface. The classic character of the mathematic model derived from this aircraft structure is piecewise-smooth dynamics system. The Po I ncar é mapping method and Floquet theory are used for the analysis the limit cycle oscillation(LCO) flutter and chaos motion of this system. The results show that the Floquet multiplier can predict the LCO flutter and periodic-k well. It also proves that the initial condition acts important influence on the dynamics character of the airfoil. The initial condition locates in the nearby the cycle orbit can lead to the LCO and the initial condition locates nearby the saddle focus orbit can lead to chaos motion,which is the main difference from most of outcomes of airfoil flutter. The figure of the Po I ncar é also approve the results.
其他文献
研究超声速及高超声速流中立方非线性机翼的极限环振荡(LCO)、分岔及颤振。首先,由活塞理论建立了二元双楔机翼的运动微分方程。然后,通过对线化系统零平衡点的特征值分析表明,系
对于由横观各向同性不可压缩的Rivlin-Saunders材料组成的球形薄膜,研究了薄膜的内、外表面在周期阶梯载荷作用下的径向振动问题.讨论了描述薄膜径向对称运动的非线性常微分方
会议
为考查基于假设模态法在时域中开展壁板非线性颤振分析的可行性,在相同的参数下,分别采用时域方法和频域方法研究了超声速飞行器壁板的非线性颤振响应,并从壁板的颤振幅值、颤振
会议
讨论了参外联合激励复合非线性振子的动力学行为。对其定常解在一阶近似下的方程进行了局部分岔分析,给出了简单分岔和Hopf分岔发生的条件,并通过对近似方程和原系统的数值模拟
在实际生物神经网络中神经元之间的连接强度是随时间变化的,本文构造了一个以Hindmarsh-Rose方程为节点动力学模型的动态变权小世界生物神经元网络模型,研究了该模型神经元的权
  白环柄菇子实体的菌盖和    菌柄洁白无瑕,菌肉浓香味美可    口。      白环柄菇野生发生在6-9 
大部分工程实际问题可以用多自由度非线性系统来描述,这些系统的数学模型是许多个耦合的两阶常微分方程。一般地,要精确求解这些方程非常困难,因此可以考虑它们的解析近似。同伦
本文用随机平均法推导出白噪声参激余维二分叉系统的标准FPK方程,通过一类特殊的参激矩阵说明扩散过程的奇异边界种类,不变测度及最大Lyapunov指数的求解方法。
In this paper,a scheme of parameter perturbation is proposed to induce transition of spiral pattern in the excitable media,which described with the modified FitzH
For CH-γ equation ut+c0ux+3uux-α(uxxt+uuxxx+2uxuxx)=-γuxxx;in order to extend the peakon solutions,we choose α and γ as bifurcation parameters to make qual-i
会议