水中多通道放电产生聚焦冲击波

P. Šunka, M. Fuciman, V. Babický, M. Člupek, J. Beneš, P. Poučková, J. Souček
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引用次数: 3

摘要

提出了一种利用水中多通道局部放电产生聚焦激波的新方法。多通道放电形成在由覆盖薄多孔陶瓷层的金属电极组成的复合阳极上。已经实现了两个版本的生成器。在第一种方法中,在直径60毫米、长100毫米的圆柱形阳极上产生圆柱形压力波。在外加电压为30 kV时,在阳极表面产生了大量几乎均匀分布的短放电通道。每个通道产生一个半球形压力波,通过所有压力波的叠加,形成一个从阳极传播的圆柱形压力波。圆柱形压力波由金属抛物面反射器(阴极)聚焦,在聚焦处附近转化为强激波。在第二种形式中,同样的多通道放电以部分球形腔的形式在复合阳极上形成收敛的球形压力波。带导电水溶液的排出物与实验空间(蒸馏水)用一层声透明膜隔开。当1 /spl μ l /F电容器组充电至30 kV时,两台发电机的焦点处冲击波幅值达到100 MPa。冲击波被尖锐地聚焦到一个3毫米的焦点区域,横向直径(最大一半的全宽度),纵向直径为40毫米。两次后续放电所产生的两个激波的相互作用已得到证实。冲击波引起的细胞损伤表现为红细胞溶血和淋巴细胞损伤。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Generation of focused shock waves by multi-channel electrical discharges in water
A novel method for generation of focused shock waves based on multi-channel partial electrical discharges in water with an increased conductivity has been developed. The multi-channel discharge is formed on a composite anode consisting of a metallic electrode covered by a thin porous ceramic layer. Two versions of the generators have been realized. In the first one a cylindrical pressure wave is created on a cylindrical anode 60 mm in diameter and 100 mm long. At the applied voltage of 30 kV, a large number of short discharge channels distributed almost homogeneously on the anode surface are initiated. Each channel creates a semi-spherical pressure wave, and by superposition of all of the waves a cylindrical pressure wave propagating from the anode is formed. The cylindrical pressure wave is focused by a metallic parabolic reflector (cathode) and near the focus it is transformed to a strong shock wave. In the second version a convergent spherical pressure wave is formed by the same kind of the multi-channel discharge on a composite anode in the form of a part of spherical cavity. The discharge volume with the conductive water solution is separated from the experimental space (distilled water) by an acoustically transparent membrane. When supplying the discharges by 1 /spl mu/F condenser bank charged to 30 kV, the amplitude of the shock wave reached 100 MPa at the focal point for the both generators. The shock waves are sharply focused to a focal area of 3 mm, in diameter transversally (full width at a half maximum) and of 40 mm longitudinally. Interaction of two shock waves generated by two subsequent discharges has been demonstrated. Cellular damage induced by the shock waves was demonstrated on hemolysis of human erythrocytes and on damage of lymphocytes.
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