共查询到17条相似文献,搜索用时 171 毫秒
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提出了采用应变模态置信度为待修正响应特征的有限元模型修正方法。应变模态置信度是评价有限元仿真与试验测试结果相关性的方法,可以为模型修正提供全局的频率误差信息和局部的应变相关性信息。首先,介绍了应变模态和有限元模型修正的相关理论方法;然后,以某航空加筋壁板结构为对象,通过仿真分析和"仿真试验"获得结构的应变模态频率以及对应的应变振型,进一步计算频率误差和应变模态置信度误差;最后,基于两种误差构造模型修正的目标函数,采用遗传算法对目标函数进行优化,修正结构中的待修正参数,并将修正后参数代入模型,验证所提方法的正确性和有效性。结果表明:所采用的方法获得的修正后有限元模型具有复现修正响应特征的能力,并且对于未修正频段内的响应也具有较好的预测能力。 相似文献
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为准确获取气体静压主轴的动力学模态特性,分别建立主轴转子及主轴部件的有限元模型,对有限元模型中添加的弹簧及电机约束边界条件进行了研究,并分别对以上两个有限元模型进行模态计算。比较两种情况下的结构固有频率、振型趋势及各阶模态下的有效参与质量,分析主轴部件中的外壳对主轴转子模态参数的影响,其中仅保留主轴转子的前六阶固有频率为1.5 Hz、277 Hz、279 Hz、316 Hz、384 Hz、385 Hz,而主轴部件的前六阶固有频率为1.5 Hz、259 Hz、270 Hz、281 Hz、352 Hz、363 Hz,以上结果中均包含刚体模态及重根模态。两者比较结果表明主轴部件的固有频率因其质量的增加而有所降低,且主轴部件不再满足对称结构形式,因而相对于仅保留主轴转子重根模态的情况有所减弱。基于有限元仿真分析结果,进一步对主轴部件进行模态试验验证,通过仿真与试验对比,结果表明主轴转子的有限元仿真结果与试验测量结果更加贴近,其前三阶误差分别为0.6%、10.6%和2.6%。上述仿真边界条件的加载与计算过程及试验测试方法对进一步提高气体静压主轴模态参数仿真精度及修正动力学仿真模型提供了有益参考。 相似文献
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针对某雷达夹具,首先系统地介绍了LMS试验模态测试方法,得到了该结构的固有频率与振型,进一步使用有限元方法计算了结构的自由模态.在此基础上,研究了仿真模态结果与试验模态结果的差异,给出了相关性分析的预处理方法,进而得到了试验模态与仿真模态的相关性结果,验证了仿真模型的有效性,为进一步的频谱分析,减少样机试验奠定基础. 相似文献
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轴流通风机叶片模态仿真及其对气动噪声的影响 总被引:1,自引:1,他引:1
利用有限元模型对叶轮模态进行了计算,判断分析了各阶模态振型对气动噪声的影响程度,求解中利用了ANSYS的模态循环对称功能,同时分析了旋转软化、应力强化对叶轮真实运转状况下模态频率的影响。 相似文献
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文中通过扩展实验模态,利用模态法思想进行形变重构,使用局部对应(Local Correspondence, LC)原理进行重构数值仿真和实验验证。该方法首先通过实验模态测试获得有限个测点的位移模态振型数据,根据实物建立较为准确的有限元模型并提取其模态数据。然后利用LC 原理选择最优的有限元位移模态振型簇对所测实验模态逐阶进行扩展。最后利用扩展后的实验模态进行重构。该方法与系统等效缩减展开过程(System Equivalent Reduction Expansion Process, SEREP)法、模态法的重构结果对比表明,该方法能够显著降低实验模态测试误差对重构精度的影响,并在有限元模型较为准确的情况下提升重构精度。 相似文献
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Accurately characterizing mid-frequency vibrations is essential for structures that require ultra-quiet vibration environments. Selecting the proper sensor locations is an important step in the model verification and validation process. State-of-the-practice approaches to sensor placement are typically based on modes shapes of the pretest finite element model. However, these modal based techniques break down in the mid-frequency range due to the high modal density. The purpose of this work was to develop a sensor placement technique based directly on a structure's frequency response. The finite element model frequency response can be decomposed into principal directions and their corresponding singular values, which relate the principal directions to the system's energy. A system's response is usually dominated by a relatively small number of principal directions, even for frequency bands with high modal densities. Principal directions are always orthogonal, while mode shapes in general are not, which makes them more robust to modeling errors and experimental noise. The new method places sensors such that the independence and signal strength of the dominant principal directions are maintained. 相似文献
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《Mechanical Systems and Signal Processing》2002,16(5):757-767
In the past few years, in-operation modal analysis has become a valid alternative for structures where classic forced vibration tests would be difficult, if not impossible, to conduct. A disadvantage of this method is that the excitation forces are unknown. Therefore, not all modal parameters can still be estimated. As a result, operational mode shape estimates remain unscaled (dependent on the unknown level of excitation) what restricts the applicability of operational modal models. So far, no techniques are available for the correct re-scaling of operational mode shapes purely based on experimental output-only data. All known methods involve either a detailed knowledge of the material characteristics of the test structure (finite element model approach) or make very restrictive assumptions about the excitation signal. In this contribution, a sensitivity-based method is proposed for the scaling of operational mode shapes on a basis of operational modal models only. 相似文献
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V.H. VuM. Thomas A.A. LakisL. Marcouiller 《Mechanical Systems and Signal Processing》2011,25(3):1028-1044
This paper presents improvements of a multivariable autoregressive (AR) model for applications in operational modal analysis considering simultaneously the temporal response data of multi-channel measurements. The parameters are estimated by using the least squares method via the implementation of the QR factorization. A new noise rate-based factor called the Noise rate Order Factor (NOF) is introduced for use in the effective selection of model order and noise rate estimation. For the selection of structural modes, an orderwise criterion called the Order Modal Assurance Criterion (OMAC) is used, based on the correlation of mode shapes computed from two successive orders. Specifically, the algorithm is updated with respect to model order from a small value to produce a cost-effective computation. Furthermore, the confidence intervals of each natural frequency, damping ratio and mode shapes are also computed and evaluated with respect to model order and noise rate. This method is thus very effective for identifying the modal parameters in case of ambient vibrations dealing with modern output-only modal analysis. Simulations and discussions on a steel plate structure are presented, and the experimental results show good agreement with the finite element analysis. 相似文献
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为了研究LHZC6/60型振动流化床干燥机主要模态的特性,对干燥机进行简化,建立有限元模型。利用有限元分析软件ANSYS对干燥机进行了模态分析,求出干燥机的前8阶固有频率和振型图。通过分析干燥机的振型图得到振动流化床干燥机的动态特性和其结构的薄弱环节,这为该机结构的改进设计和动态分析提供了理论依据。 相似文献
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Identification, localization and quantification of structural damage can be performed through a model-updating procedure. Model-updating methods require a baseline finite element (FE) model of the undamaged structure, which imposes a restriction on their applicability and can become very problematic especially for large and complex civil structures. Modeling errors in the baseline model whose effects exceed the modal sensitivity to damage are critical and make an accurate estimation of damage impossible. This paper presents an identification algorithm using modal data for assessing structural damage that is based on FE-updating procedures and takes modeling error into account. To overcome its influence, differences of mode shapes and frequencies before and after damage for both numerical model and experimental measurements are used instead of the mode shapes and frequencies themselves. To formulate the objective function, two different approaches have been considered taking into account how these differences are grouped: a single-objective approach and a multiobjective approach. The effectiveness of both approaches is verified against numerical and experimental results. 相似文献