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Probing Fiber Orientation in Composite Laminates Using EMATs

机译:使用EMAT探索复合材料层压板中的纤维取向

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Due to the highly anisotropic elastic properties of the plies in a fiber-reinforced composite laminate, transverse (shear) waves propagated through the laminate carry rich information about the fiber orientation and ply stacking sequence in the laminate. Such signals can therefore be used in the nondestructive detection of ply lay-up or stacking sequence errors in composite laminates. Several attempts have been reported for exploiting the strong interaction between shear wave polarization and fiber orientation for nondestructive evaluation (NDE) purposes. For example, Hsu et al [2, 5] have used contact shear wave transducers in a "crossed polarizer" configuration in which the polarization directions of the transmitter and receiving transducers on the two faces of the laminate were perpendicular to each other and both were rotated in unison over a full circle. The transmitted signal was found to have good sensitivity for certain ply orientation and stacking sequence anomalies. An experimental problem with making reproducible shear wave measurements is the need for a shear wave couplant. Keeping the coupling condition constant is especially problematic for measurements that require frequent change of the angular orientation of the shear wave transducers. To alleviate this problem, researchers at Iowa State University used EMAT probes for the generation and detection of normal incidence shear waves in a non-contact manner. The composite sample was sandwiched between two aluminum blocks and the EMAT probes were placed on the outside faces of the two blocks. The EMATs can be rotated freely with computer-controlled stepping motors in an angular scan. For uncured laminates, the pressure applied on the blocks was sufficient for shear waves to transmit through. For solid cured laminates, shear couplant was still used between its surfaces and the aluminum; however, the coupling condition was not disturbed by rotation and hence remained constant. In an angular scan, the transmitted shear wave signals at every angular position were acquired. After a full-circle scan, an image as function of angle and time was obtained. Such "angle-time" patterns, especially for the crossed configuration, were found to be very characteristic to the ply lay-up of the laminate and can be used to check errors in ply orientation and stacking sequence in composite laminates effectively. Recently a complete analytical model was also developed by Fei and Hsu for the propagation of shear waves in composite laminates. The analytical model led to a result that is very compact and tractable. The model took into account all the reflected waves at the interfaces in the laminate by including the four partial waves in each layer that are polarized parallel to and perpendicular to the fiber, and propagating in the forward and reversed directions. The incident and transmitted shear waves components were found to be related by four transfer functions, which can be determined experimentally for a given laminate by four measurements, with the transmitter angle and receiver angle at (0, 0), (0, 90), (90, 0), and (90, 90). The model has been experimentally verified using both cured and uncured laminates.
机译:由于纤维增强的复合层压板中的帘布层具有高度各向异性的弹性,因此传播通过层压板的横向(剪切)波会携带有关层压板中纤维取向和帘布层堆叠顺序的丰富信息。因此,此类信号可用于无损检测复合材料层压板中的板层铺放或堆叠顺序错误。为了无损评估(NDE)目的,已经报道了几种尝试利用剪切波偏振和纤维取向之间的强相互作用的尝试。例如,Hsu等人[2,5]在“交叉偏振器”配置中使用了接触剪切波换能器,其中层压板两个面上的发射器和接收器的极化方向彼此垂直,并且两个方向均为一致地旋转了一整圈。发现所传输的信号对于某些层定向和堆叠序列异常具有良好的灵敏度。进行可重复的剪切波测量的实验问题是需要剪切波耦合剂。对于需要频繁改变剪切波换能器的角度方向的测量,保持耦合条件恒定尤其成问题。为了缓解这个问题,爱荷华州立大学的研究人员使用EMAT探头以非接触方式生成和检测法向入射切变波。将复合材料样品夹在两个铝块之间,并将EMAT探针放置在两个铝块的外面。 EMAT可以通过计算机控制的步进电机在角度扫描中自由旋转。对于未固化的层压板,施加在块上的压力足以使剪切波通过。对于固体固化的层压板,仍然在其表面和铝之间使用剪切耦合剂。但是,耦合条件不受旋转的干扰,因此保持恒定。在角扫描中,获取在每个角位置处传输的剪切波信号。经过全圆扫描后,获得的图像是角度和时间的函数。发现这种“角-时间”图案,特别是对于交叉构型,对于层压板的层板铺放是非常有特征的,并且可以用于有效地检查复合层压板中的板层取向和堆叠顺序的误差。最近,Fei和Hsu还开发了一个完整的分析模型,用于在复合材料层压板中传播剪切波。分析模型得出的结果非常紧凑且易于处理。该模型通过在每一层中包括平行于和垂直于光纤极化的四个部分波,并在正向和反向传播,从而考虑了层压板界面处的所有反射波。发现入射和透射切变波分量与四个传递函数相关,可以通过四个测量实验对给定的层压板进行实验确定,发射角和接收角分别为(0,0),(0,90), (90,0)和(90,90)。该模型已使用固化和未固化的层压板进行了实验验证。

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