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Effect of the Test Basket on Lithotripter Shock Waves, Cavitation Field, and Stone Breakage

机译:试验篮对岩石冲击波,空化场和石打破的影响

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The performance of shock wave (SW) lithotripters is often assessed by measuring the breakage efficiency of model stones. Such in vitro tests are usually performed by positioning the stones in plastic mesh baskets. We asked if the plastic mesh affects the properties of SWs, and whether this alteration influences cavitation fields and stone breakage efficiency. Experiments were conducted using a research electrohydraulic lithotripter patterned after the Dornier HM3 (HM3-clone), and a clinical electromagnetic lithotripter (XX-ES). Shock waves were measured at the geometric focus (F2) of the HM3-clone lithotripter using a fiber-optic probe hydrophone (FOPH-500). A 2.5x4mm extruded polypropylene mesh was positioned-8mm or-40mm prefocally. Cavitation bubbles were recorded using a multiframe high-speed camera (Imacon 468). Breakage of gypsum cement stones was assessed using the XX-ES lithotripter. SWs generated by this lithotripter propagate downward, so that when stones were positioned in an open-top basket, SWs could reach the stone without passing through the mesh that held the stone. This was compared to a mesh basket in the form of a cylinder, with which SWs had to pass through the mesh to reach the stone. Acoustic measurements showed that the mesh had little effect on the leading positive-pressure phase of the SW, but attenuated to some degree the tensile component of the pulse. Proximity of the mesh to F2 affected the waveforms such that the mesh positioned at 40mm prefocally was almost acoustically transparent, but the effect was much more pronounced when the mesh was within several millimeters of F2. High-speed camera images showed that cavitation was reduced beyond the mesh. Stone breakage was less efficient when SWs had to pass through the mesh to reach the stone. When SWs had to pass through the mesh, the number of SWs to break stones was 634-125 SWs, which was greater (P<0.002) than the 448-44 SWs needed to break stones in the open-top basket. These findings show that mesh material-generally considered to be acoustically "invisible"-may have a measureable effect on lithotripter SWs, cavitation fields, and stone breakage efficiency. These factors should be kept in mind when interpreting in vitro test results, particularly in studies assessing the performance of SW lithotripters or in studies on the mechanisms of SW action.
机译:通过测量模型结石的破损效率,通常评估冲击波(SW)型碎石梯的性能。这种体外测试通常通过将石头定位在塑料网篮中来进行。我们询问塑料网格是否会影响SWS的性质,以及这种改变是否会影响空化场和石头破损效率。使用Dornier HM3(HM3-Clone)和临床电磁型材(XX-ES)图案化的研究电液型碎石钳进行实验。使用光纤探针水听器(FOPH-500)在HM3-CLONE LITHOTRIPTER的几何焦点(F2)处测量冲击波。将2.5x4mm挤出的聚丙烯网定位为8mm或-40mm。使用多帧高速摄像头(Imacon 468)记录空化泡沫。使用XX-ES Lithotrapter评估石膏水泥结石的破损。由此碎石提示者产生的SWS向下传播,因此当石头定位在敞篷篮中时,SWS可以到达石头而不通过夹住石头的网。将其与圆柱体形式的啮合篮进行比较,SWS必须穿过网状物到达石头。声学测量表明,网格对SW的前导正压相的影响几乎没有影响,但衰减到脉冲的抗拉部件的一定程度。网格到F2的接近影响波形,使得位于40mm的网格相当几乎声学透明,但是当网状物在几毫米的F2内时,效果要明显。高速相机图像显示空化减少到网状物之外。当SWS必须穿过网状物到达石头时,石头破损效率较低。当SWS不得不通过网格时,SWS的数量是634-125瑞斯,比448-44 SWS更大(P <0.002),所需的448-44 SWS在敞篷篮中打破石头。这些发现表明,网格材料 - 通常被认为是声学上的“看不见的” - 可以对碎石的SWS,空化场和石头破损效率具有可测量的影响。在解释体外测试结果时,应牢记这些因素,特别是在评估SW Lithotriper的性能或研究SW行动机制的研究中。

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