Birer A, Ghohestani M, Cathignol D
INSERM, Unit 556, 151 Cours Albert Thomas, Lyon Cedex 03 69424, France.
Ultrason Sonochem. 2004 May;11(3-4):155-60. doi: 10.1016/j.ultsonch.2004.01.012.
New clinical concepts in lithotripsy demand small shock heads. Reducing the size of piezoelectric shock heads will only be possible if the pressure generated at the surface of each transducer can be increased so that, the total pressure at the focus remains very high. So, we propose a new method allowing the generation of large surface pressures. It is well known that the piezoelectric rods in piezocomposite material are more fragile in the extension mode than in the compression mode. For this reason, actuators are mechanically pre-stressed between two flasks. This method cannot be used for transducers working at high frequencies, about 0.5 MHz. For this reason, we proposed to electrically pre-strain the piezoelectric material by applying high electric field in the opposite direction of the polarisation. In a first mode we proposed to pre-strain in continuous mode the transducer. Unfortunately we noticed a rapid de-poling and re-poling in the inverse direction. In a second mode to reduce depolarisation, this field was applied only during a short time just before the generation of the pulse which generate the compressive wave and in a third mode, the transducer was re-poled between two successive electrical pulses. Using this last method, it was possible to increase the maximum pressure at the surface of a 20 mm diameter plane piston to 20% and reach 4 MPa. According to this idea a very compact shock wave generator was designed. The generator made of a 1-3 piezocomposite material has a diameter of 120 mm and focused at 120 mm. The maximum pressure and the width of the compressive wave at the focus were, respectively, 60 MPa and 1.5 micros. The focal zone measured at -3 dB is an ellipsoid 6 mm high in the propagating axis and 3 mm width in the perpendicular direction. The efficacy of this generator was measured as the number of shocks necessary to totally disintegrate plaster balls 15 mm in diameter mimicking the kidney stones. At full power the number of shocks was only 150 which is rather the same number as the one obtained using electrohydraulic machine generally considered as the gold standard. This results show that piezoelectric material may be advantageously used for the manufacturing of shock wave generators.
碎石术的新临床概念需要小型冲击波源。只有当每个换能器表面产生的压力能够增加,从而使焦点处的总压力保持在很高水平时,减小压电冲击波源的尺寸才有可能实现。因此,我们提出了一种能够产生高表面压力的新方法。众所周知,压电复合材料中的压电棒在拉伸模式下比压缩模式下更脆弱。因此,在两个烧瓶之间对致动器施加机械预应力。这种方法不适用于工作频率约为0.5MHz的换能器。因此,我们建议通过在与极化相反的方向施加高电场来对压电材料进行电预应变。在第一种模式中,我们建议对换能器进行连续模式的预应变。不幸的是,我们注意到换能器迅速反向去极化和再极化。在第二种模式中,为了减少去极化,该电场仅在产生压缩波的脉冲之前短时间内施加,而在第三种模式中,在两个连续的电脉冲之间对换能器进行再极化。使用最后一种方法,可以将直径为20mm的平面活塞表面的最大压力提高20%,达到4MPa。基于这一理念,设计了一种非常紧凑的冲击波发生器。该发生器由1-3型压电复合材料制成,直径为120mm,聚焦距离为120mm。焦点处的最大压力和压缩波宽度分别为60MPa和1.5微秒。在-3dB处测量的焦区是一个椭球体,在传播轴上高6mm,在垂直方向上宽3mm。该发生器的效能通过将模拟肾结石的直径15mm的石膏球完全粉碎所需的冲击次数来衡量。在全功率下,冲击次数仅为150次,这与通常被视为金标准的液电式设备所获得的冲击次数相当。这些结果表明,压电材料可有利地用于制造冲击波发生器。