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首页> 外文期刊>Physics of plasmas >Study and optimization of negative polarity rod pinch diode as flash radiography source at 4.5 MV
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Study and optimization of negative polarity rod pinch diode as flash radiography source at 4.5 MV

机译:4.5 MV负电极棒状夹点二极管作为闪光放射源的研究与优化

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摘要

The negative polarity rod pinch diode (NPRPD) is a potential millimeter spot size radiography source for high voltage generators (4 to 8 MV) [Cooperstein, "Considerations of rod-pinch diode operation in negative polarity for radiography", in Proceedings of the 14th IEEE Pulsed Power Conference, 2003, pp. 975-978]. The NPRPD consists of a small diameter (few mm) cylindrical anode extending from the front end of the vacuum cell through a thin annular cathode, held by a central conductor. The polarity has been inverted when compared to the original rod pinch diode [Cooperstein, et al., "Theoretical modeling and experimental characterization of a rod-pinch diode", Phys. Plasmas 8(10), 4618-4636 (2001)] in order to take advantage from the maximal x-ray emission toward the anode holder at such a voltage [Swanekamp, et al., "Evaluation of self-magnetically pinched diodes up to 10 MV as high resolution flash X-ray sources", IEEE Trans. Plasma Sci. 32(5), 2004-2016 (2004). We have studied this diode at 4.5 MV, driven by the ASTERIX generator [Raboisson, et al., "ASTERIX, a high intensity X-ray generator", in Proceedings of the 7th IEEE Pulsed Power Conference, 1989, pp. 567-570.]. This generator, made up of a capacitor bank and a Blumlein line, was initially designed to test the behavior of electronic devices under irradiation. In our experiments, the vacuum diode has been modified in order to set up flash a radiographic diode [Etchessahar, et al., "Negative polarity rod pinch diode experiments on the ASTERIX generator", in Conference Records-Abstracts, 37th IEEE International Conference on Plasma Science, 2010]. The experiments and numerical simulations presented here allowed the observation and analysis of various physical phenomena associated with the diode operation. Also, the influence of several experimental parameters, such as cathode and anode diameters, materials and surface states, was examined. In order to achieve the most comprehensive characterization of the diode, both optical and x-ray diagnostics were used, including high speed multi-image ICCD (intensified CCD) cameras, streak camera, dosimeters, spot size measurements, and pinhole cameras. A set of new results have been obtained through this study. The plasma emission from the anode and cathode surfaces and its expansion appear to be critical for the diode functioning. Also, for the first time, potential sources of diode instability were identified. Finally, an optimal and stable diode configuration was found with the following parameters: 52 rad at 1 m (in Al) and 2.2 mm spot size.
机译:负极杆夹二极管(NPRPD)是高压发生器(4至8 MV)的潜在毫米点尺寸放射线照相源[Cooperstein,“放射线照相中负极杆捏二极管的注意事项”,第14卷,第14页IEEE脉冲功率会议,2003年,第975-978页]。 NPRPD由小直径(几毫米)的圆柱形阳极组成,该阳极从真空室的前端延伸穿过一个薄的环形阴极,该阴极由中心导体固定。与原始的棒状捏二极管相比,极性已经反转了[Cooperstein等人,“棒状捏二极管的理论模型和实验特性”,Phys。等离子8(10),4618-4636(2001)],以利用在这样的电压下向阳极支架的最大X射线发射中获益[Swanekamp等人,“自磁性夹层二极管的评估10 MV作为高分辨率闪光灯X射线源”,IEEE Trans。等离子科学32(5),2004-2016(2004)。在1989年第7届IEEE脉冲功率会议的论文集中,我们研究了由ASTERIX发生器驱动的4.5 MV二极管[Raboisson等,“ ASTERIX,高强度X射线发生器”,第567-570页。 。]。该发生器由电容器组和Blumlein线组成,最初设计用于测试电子设备在辐射下的行为。在我们的实验中,对真空二极管进行了修改,以设置闪光射线照相二极管[Etchessahar等,“第37届IEEE国际会议的会议记录摘要”上的“ ASTERIX发生器上的负极杆夹二极管实验”。等离子体科学,2010年。此处提供的实验和数值模拟可以观察和分析与二极管工作相关的各种物理现象。此外,检查了几个实验参数的影响,例如阴极和阳极的直径,材料和表面状态。为了实现二极管的最全面的表征,光学和X射线诊断都被使用,包括高速多图像ICCD(增强CCD)相机,条纹相机,剂量计,光斑尺寸测量和针孔相机。通过这项研究获得了一组新的结果。来自阳极和阴极表面的等离子体发射及其膨胀对于二极管的功能似乎至关重要。同样,首次确定了二极管不稳定的潜在原因。最后,找到了具有以下参数的最佳且稳定的二极管配置:1 m(在Al中)为52 rad,光斑大小为2.2 mm。

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