Prego Borges J L, Montero de Espinosa F, Salazar J, Garcia-Alvarez J, Chávez J A, Turó A, Garcia-Hernandez M J
Sensor Systems Group, Electrical Engineering Department, Universitat Politecnica de Catalunya, C/Jordi Girona, 1-3, Modulo C4, 08034 Barcelona, Spain.
Ultrasonics. 2006 Dec 22;44 Suppl 1:e667-72. doi: 10.1016/j.ultras.2006.05.125. Epub 2006 Jun 6.
Air coupled piezoelectric ultrasonic array transducers are a novel tool that could lead to interesting advances in the area of non-contact laminar material testing using Lamb wave's propagation techniques. A key issue on the development of such transducers is their efficient coupling to air media (impedance mismatch between the piezoelectric material and air is 90 dB or more). Adaptation layers are used in order to attain good matching and avoid possible serious signal degradation. However, the introduction of these matching layers modify the transducer surface behaviour and, consequently, radiation characteristics are altered, making the usual idealization criteria (of uniform surface movement) adopted for field simulation purposes inaccurate. In our system, we have a concave linear-array transducer of 64 elements (electrically coupled by pairs) working at 0.8 MHz made of PZ27 rectangular piezoceramics (15 mm x 0.3 mm) with two matching layers made of polyurethane and porous cellulose bonded on them. Experimental measurements of the acoustic aperture of single excited array elements have shown an increment on the geometrical dimensions of its active surface. A sub-millimeter vibrometer laser scan has revealed an extension of the aperture beyond the supposed physical single array element dimensions. Non-uniform symmetric apodized velocity surface vibration amplitude profile with a concave delay contour indicates the presumed existence of travelling wave phenomena over the surface of the outer array matching layer. Also, asymptotic propagation velocities around 2500 m/s and attenuation coefficient between 15 and 20 dB/mm has been determined for the travelling waves showing clear tendencies. Further comparisons between the experimental measurements of single array element field radiation diagram and simulated equivalent aperture counterpart reveal good agreement versus the ideal (uniform displaced) rectangular aperture. For this purpose an Impulse Response Method (IRM) has been used.
空气耦合压电超声阵列换能器是一种新型工具,有望在利用兰姆波传播技术进行非接触层状材料测试领域取得有趣的进展。开发此类换能器的一个关键问题是它们与空气介质的有效耦合(压电材料与空气之间的阻抗失配为90分贝或更高)。为了实现良好的匹配并避免可能的严重信号退化,使用了适配层。然而,这些匹配层的引入改变了换能器的表面行为,因此辐射特性也发生了变化,使得用于场模拟目的的通常理想化标准(均匀表面运动)不准确。在我们的系统中,我们有一个由64个元件(成对电耦合)组成的凹面线性阵列换能器,工作频率为0.8兆赫,由PZ27矩形压电陶瓷(15毫米×0.3毫米)制成,上面粘结有两层由聚氨酯和多孔纤维素制成的匹配层。对单个激发阵列元件的声孔径进行的实验测量表明,其有效表面的几何尺寸有所增加。亚毫米级激光振动计扫描显示,孔径扩展超出了假定的物理单个阵列元件尺寸。具有凹面延迟轮廓的非均匀对称变迹速度表面振动幅度分布表明,在外阵列匹配层表面可能存在行波现象。此外,已确定行波的渐近传播速度约为2500米/秒,衰减系数在15至20分贝/毫米之间,呈现出明显的趋势。单个阵列元件场辐射图的实验测量结果与模拟等效孔径对应结果之间的进一步比较表明,与理想(均匀位移)矩形孔径相比,二者吻合良好。为此,使用了脉冲响应方法(IRM)。