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典型静电放电火花点燃能力测试研究 总被引:1,自引:1,他引:0
通过对静电放电火花点火过程的物理特征研究,分析与总结了典型静电放电火花的点燃能力.根据放电火花的产生条件和形状特点,静电放电火花分为电晕放电、刷形放电、料仓堆表面放电、人体放电、火花放电和传播型尉形放电6种典型放电类型.根据静电放电火花的火花空间分布范围和火花持续时间,研究了静电放电火花点燃可燃物的能力.典型静电放电火花的实际点火能量为:电晕放电不大于0.025mJ,刷形放电不大于3mJ,料仓堆表面放电不大于10mJ.人体放电不大于30mJ,火花放电不大于1J,传播型刷形放电不大于10J. 相似文献
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为了使雷电电磁场的计算更加接近实际情况,并对远场区雷电电磁脉冲场进行模拟,利用偶极子理论对斜向放电通道雷电电磁场解析表达式进行了求解,用解析方法对地表雷电电磁场及其导数在远场区的一阶、二阶近似表达式进行了推导,得到了电磁场及其导数与通道底部电流及其导数的远场近似关系。采用脉冲函数表示通道基电流,对比了精确表达式与近似表达式计算的电磁场及其导数波形。结果表明在远场区,斜向通道雷电电磁场波形与其近似波形的偏差、电磁场导数波形与其近似导数波形之间的偏差均随着距离的增加而减小,且电磁场导数近似公式要比电磁场近似公式适用范围更加广泛。计算结果验证了解析推导近似的可行性。 相似文献
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为了使雷电电磁场的计算更加接近实际情况,并对远场区雷电电磁脉冲场进行模拟,利用偶极子理论对斜向放电通道雷电电磁场解析表达式进行了求解,用解析方法对地表雷电电磁场及其导数在远场区的一阶、二阶近似表达式进行了推导,得到了电磁场及其导数与通道底部电流及其导数的远场近似关系。采用脉冲函数表示通道基电流,对比了精确表达式与近似表达式计算的电磁场及其导数波形。结果表明在远场区,斜向通道雷电电磁场波形与其近似波形的偏差、电磁场导数波形与其近似导数波形之间的偏差均随着距离的增加而减小,且电磁场导数近似公式要比电磁场近似公式适用范围更加广泛。计算结果验证了解析推导近似的可行性。 相似文献
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任何物体内部都带有电荷,一般状态下,其正、负电荷数量相等,对外不显出带电现象,但当两种不同物体接触或摩擦时,物体中的电子会越过界面,进入另一种物体内,产生静电。因它们所带电荷发生积聚时产生了很高静电压,当带有不同电荷的两个物体分离或接触时出现电火花,这就是静电放电现象。静电火灾是由静电放电而形成的,静电火灾成因非常复杂,给预防静电火灾发生带来了困难;但如明确其产生的条件,对静电火灾的防止具有一定的意义。静电火灾的形成主要由于同时具备以下条件而引起。一、产生静电的条件静电起电是物质在相互接触过程中电荷的分离和转移造成的。 相似文献
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J. Odeurs 《Hyperfine Interactions》2001,135(1-4):155-166
The frequency spectrum of electromagnetic radiation can be written as the Fourier transform of the first-order correlation
function of the vector potential. If nuclei are coupled to the radiation field, the Heisenberg equations of motion of the
field operators contain nuclear operators and vice versa. Under plausible assumptions the equations of motion for the nuclear
operators can be integrated and hence, the equations of the field operators can be solved. The vector potential of the radiated
field can then be expressed as a function of solely nuclear quantities. The first-order correlation function deduced from
it contains only two-times and one-time averages of simple nuclear creation and annihilation operators. The theory can be
used to explain homogeneous line broadening for long-lived nuclei submitted to small fluctuating interactions.
This revised version was published online in July 2006 with corrections to the Cover Date. 相似文献
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Modeling technique for electromagnetic fields excited by antennas is an important topic in computational electromagnetics, which is concerned with the numerical solution of Maxwell's equations. In this paper, a novel hybrid technique that combines method of moments(MoM) with finite-difference time-domain(FDTD) method is presented to handle the problem. This approach employed Huygen's principle to realize the hybridization of the two classical numerical algorithms. For wideband electromagnetic data, the interpolation scheme is used in the MoM based on the dyadic Green's function. On the other hand, with the help of equivalence principle, the scattered electric and magnetic fields on the Huygen's surface calculated by MoM are taken as the sources for FDTD. Therefore, the electromagnetic fields in the environment can be obtained by employing finite-difference time-domain method. Finally, numerical results show the validity of the proposed technique by analyzing two canonical samples. 相似文献
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研究了静电放电(ESD)人体模式(HBM)下的脉冲应力对有机发光二极管(OLED)的性能及寿命的影响,并讨论了相应的物理机制。对比分析了4组OLED在施加ESD放电为0,200,800,1 600 V前后的电学和光学特性,并进行了相应的寿命测试分析。研究发现,OLED器件的光谱对ESD不敏感,随着冲击电压的增大,由于静电打击对载流子的短期抑制效应,OLED的亮度出现轻微下降。在静电冲击电压为200 V和800 V时,伏安特性没有发生变化;当静电冲击电压增至1 600 V时,反向漏电有明显增加。后续的加速寿命实验表明,静电打击对器件的工作寿命没有明显的规律性影响,但是会一定程度提高非本质老化失效的概率。 相似文献
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We apply Campolattaro's spinor representation of the electromagnetic field to noncommutative spaces. The spinor representation of the (self-dual) electromagnetic field on noncommutative spaces is obtained. 相似文献
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旋转磁场作用下磁流变液颗粒运动及结构演化的模拟 总被引:9,自引:1,他引:8
通过对旋转磁场作用下磁流变液一定数目颗粒运动的数值模拟,在旋转平面内得到盘状聚集结构,在垂直于旋转平面的平面内得到层状结构,得出旋转磁场作用下磁流变液的结构特点。在模拟过程中颗粒受到磁场作用力简化为磁偶极子间相互作用。 相似文献
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采用壳模型分析了深空核爆的电子运动规律,对深空核爆电磁脉冲的形成机理进行了初步研究。考虑MeV量级出射电子的相对论效应,在相对论框架下进行了电子运动过程的推导。计算了空间电荷层限制的形成时间,并提出一旦形成空间电荷限制,后续状态满足准静态近似条件。在此基础上,推导了空间电荷振荡的频率,并与半数值计算的结果进行比对,二者符合得较好。计算表明,远场达到峰值的时间与爆炸当量、电子初始动能和弹体半径等参数密切相关,电场峰值总是出现在核反应极大值之前,并且在空间电荷层限制的形成时间附近。 相似文献
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The survey analysis capabilities of spark source mass spectrography have proved to be very important in the determination of very low concentrations of elements in nonconductors and semiconductors. Some of the methods devised for the special handling and sparking of the poor conductors have been reviewed by Guthrie1. In general, attempts to initiate and sustain a radio frequency spark between nonconductor self-electrodes require inconviently high spark voltages and considerable operator time and attention. Moreover, the low ion yields often characteristic of the nonconductor self-electrode spark compel exposure times commonly in excess of one hour for exposure levels requisite for the detection of impurities at 1 part-per-million concentrations. 相似文献