GJB151B CS115的电路仿真分析(一)--校准设备指标需求分析北大核心CSCD

GJB151B CS115给出了开展脉冲传导敏感度试验的校准平台构成和校准波形标准,但未明确校准平台各设备(脉冲源、电流注入环、校准夹具等)的具体指标需求。为解决这一问题,本文在前期脉冲电流注入电路仿真研究工作的基础上,构建了校准平台的时域电路模型,通过逐一改变模型参数的方法,仿真分析了脉冲源内部回路电感、电流注入环等效电感/电阻/电容等对校准波形前沿、半宽以及平顶降的影响,得出了平台各设备应达到的技术指标。该工作是对GJB151B CS115的有益补充,为搭建CS115试验平台,开展电子设备脉冲传导敏感度试验提供了技术支撑。     

微型动态级联爆磁压缩发生器研究

为满足某强电磁脉冲辐射系统对轻小型脱离地面脉冲电源的应用需求,研究了一种微型动态级联爆磁压缩发生器。首先介绍了该发生器的结构参数,然后利用基于等效电路的数值计算模型对该发生器电路参数和输入输出电流进行了模拟计算,最后以蓄电池供电的初始能源为发生器提供初始种子电流,对发生器输出特性进行了爆轰实验。实验结果表明,发生器在1.44 μH电感负载上产生脉冲电流峰值达到49 kA,电流上升时间5.2 μs,能量放大约7.8倍。     

紧凑环注入系统高压脉冲电源设计

以放电回路理论模型计算和仿真分析为指导,设计了紧凑环注入装置(CTI)高压脉冲电源,并在CTI上进行放电实验。实验结果证明所设计的CTI高压脉冲电源可产生特定频率下100kA的目标电流,保证了CTI成型场及加速场电极的供电需求。     

强流离子源灯丝电源设计与分析

灯丝电源是中性束注入器等离子体发生器电源系统的重要组成部分,为了满足其低电压大电流输出特性要求,提出了带平衡电抗器双反星形整流电路的拓扑结构的电源设计方案。该拓扑结构与三相桥式整流电路相比较在采用相同器件下可达到更高功率,减少交流侧输入电流谐波并提高功率因素。分析了该拓扑结构下整流输出特性和所含的谐波分量,根据设计指标计算了整流变压器和平衡电抗器的相关参数,最后通过仿真和实验结果验证了这一拓扑结构的可行性。     

GJB151B CS115的电路仿真分析（二）——标准应用分析

为解决GJB151B CS115电缆束注入脉冲传导敏感度测试项目中的试验设计、效果预估等问题,在介绍不同类型受试线缆感性脉冲电流注入电路模型的基础上,仿真分析了试验设置中的各项因素（线缆设置、末端负载等）对注入到受试设备端口耦合电流/电压的影响,得到了CS115试验设置中存在的一些规律性特征,给出了应用电路仿真开展CS115试验设置分析和优化的方法。     

大电流纳秒级脉宽激光二极管驱动电路的设计

脉冲激光雷达探测的性能直接与激光束的质量和能量有关,而激光驱动电路则直接决定了脉冲激光的功率和脉冲宽度。基于半导体激光雷达探测系统的要求,设计出应用于激光雷达发射系统的大电流纳秒级脉冲半导体激光二极管的驱动电路。介绍了电路的系统结构和驱动级电路的模型及其理论分析,推导其电流数学模型计算公式,并对关键器件的选择进行了总结;运用SPICE仿真程序对驱动电路进行了仿真。制作了印刷电路板,得到峰值电流25A,脉宽15ns的脉冲电流,满足设计要求。     

一种高压电源谐振升压倍压电路

提出了一种高压电源谐振升压倍压电路,该电路由LC谐振电路与整流电路组成。对该电路的工作模式和稳态输出特性进行了分析;建立了该电路的数学模型:以归一化的形式定量描述了稳态输出电压与电流的增益、短路特性和开路特性、输出纹波与电压降、以及器件上的电应力,并分析了电路品质因数、归一化频率和电容比对输出特性的影响;对该电路进行了仿真与实验研究,仿真结果与实验结果具有很好的一致性,验证了数学模型的正确性。与C-W电路的对比研究结果表明:所提出的电路具有输出电压稳定、输出纹波小、短路特性好以及响应速度快的优点,满足高压小电流的应用需求。     

双指数脉冲电流发生器的电路仿真计算

双指数脉冲电流发生器可用于电子系统端口传导耦合实验,主要用于研究电磁敏感器件的电磁脉冲效应的损伤规律。根据实验要求,该发生器能够输出前沿10 ns、脉宽100 ns、电流幅值3 kA的双指数脉冲电流。建立了该发生器的电路模型,并对杂散电容和电感对输出电流波形的影响进行了分析。模拟计算表明,电流信号的过冲现象和后沿叠加干扰信号的原因可能是电阻负载自身存在的杂散电容和测量电流的线圈附近的杂散电容和电感的共同作用导致的。经过理论计算,如果在测量线圈附近添加适当的滤波设备或者用无损同轴电缆引出电流,能够明显地抑制过冲和干扰。     

集成门极换流晶闸管电学模型的优化及参数提取

在集成门极换流晶闸管(IGCT) 2T-3R-C 电学模型的基础上,针对其模型关断电压出现与实测波形不 符的振荡问题,建立了一种 IGCT 改进电学模型,并提出一套可用于改进电学模型的参数提取方法,给出改进电 学模型电路结构和器件参数。将模型的动态特性仿真结果与 4kA/4.5kV 型号 IGCT 的 4kA/4.5kV 等级实验结果、 3.5kA/4.5kV 等级实验结果以及现有 2T-3R-C 模型仿真结果进行对比,验证了改进电学模型的准确性、适用性、 优越性。      

光发射模块的实现及直线感应加速器注入器的模拟

本文研究开发直线感应加速器的光发射模块,并验证该模块的正确性.首先建立光发射模型,该模型确立阴极参数和入射激光与宏粒子初始值间的关系,并将该模型实现到代码中;其次,根据实验参数建立注入器模型,模拟光阴极的发射过程;最后,将模拟结果与实验结果比较,发现模拟的发射电流与实验电流吻合,发射度与理论分析一致,验证了模拟的正确性.     

脉冲电流探头的时域标定研究

 介绍了一种Rogowski线圈脉冲电流探头时域标定和标定数据处理的方法，将脉冲法时域标定的结果和频域标定结果进行了比较。针对电流探头的低频失真，采用系统辨识方法建立了测量系统的动态模型，并对探头输出信号的失真进行校正。实测数据验证了所建模型的有效性，设计出的数字补偿滤波器可将测量系统校正为一理想的比例环节。     

快脉冲高电压大电流测量探头标定方法

基于脉冲形成原理提出了一种快脉冲高电压大电流测量探头的在线标定方法。利用闪光二号加速器输出线和二极管作为脉冲形成线,结合研制的低电感开关和负载,产生一个前沿小于3 ns、脉宽20 ns的准方波,对二极管电压测量探头微分型电容分压器和电流测量探头微分环进行了在线标定,得到测量探头在实际使用环境中的时间响应小于4 ns。该方法消除了非在线标定环境和实际环境无法统一对标定结果的影响,可推广应用于传输线型脉冲功率装置的探头标定。     

Plasma shape optimization for EAST tokamak using orthogonal method

It is necessary to reduce the currents of poloidal field(PF) coils as small as possible, during the static equilibrium design procedure of Experimental Advanced Superconductive Tokamak(EAST). The quasi-snowflake(QSF) divertor configuration is studied in this paper. Starting from a standard QSF plasma equilibrium, a new QSF equilibrium with 300 kA total plasma current is designed. In order to reduce the currents of PF6 and PF14, the influence of plasma shape on PF coil current distribution is analyzed. A fixed boundary equilibrium solver based on a non-rigid plasma model is used to calculate the flux distribution and PF coil current distribution. Then the plasma shape parameters are studied by the orthogonal method. According to the result, the plasma shape is redefined, and the calculated equilibrium shows that the currents of PF6 and PF14 are reduced by 3.592 kA and 2.773 kA, respectively.     

Modelling of optical Kerr effects on the static and dynamic behaviors of quantum cascade laser

The effect of optical Kerr nonlinearity on the static and dynamic behaviors of quantum cascade laser operating in the mid-infrared is theoretically investigated. Our model is based on three-level rate equations including the dependence of the loss on photon number in the cavity. The optical stability domain that allows for the determination of current injection is derived within the premises of our model. The analytical solutions of eigenvalue equation allowing the investigation of stability analysis are obtained. Furthermore, nonlinear effects influence significantly the dynamics of photons in cavity and electrons in the upper laser level.     

Demonstration of plasma startup by coaxial helicity injection

The first successful results on the transfer of a coaxial helicity injection (CHI) produced discharge to inductive operation are reported. CHI-assisted plasma startup is more robust than inductive only operation. After hand off for inductive operation, the initial 90 kA of CHI-produced current drops to 40 kA, then ramps up to 170 kA, using only 30 mV s, more than 30% higher than that produced by induction alone. These significant performance enhancing results were obtained on the HIT-II spherical torus experiment (major/minor radius of 0.3/0.2 m).     

Time Dependence of Anode Spot Formation Threshold Current in Vacuum Arcs

The variation of threshold current for the transition between the low current quiescent vacuum arc mode, and the high voltage noisy mode associated with anode spot formation, was measured as a function of peak current, current waveform frequency, and electrode separation on fixed diameter (25 mm) Cu and Ni electrodes. At current waveform frequencies of about 60 Hz on Cu electrodes, the threshold current depends mainly on electrode spacing, as has been observed by other investigators. However, at higher waveform frequencies, the threshold current becomes a strong function of peak current as well. At 347 Hz on 25 mm. diam. Cu electrodes separated by 10 mm, the threshold current rose from approximately 2 kA to 5.5 kA, as the peak current rose from 2 kA to 6 kA. At 543 Hz on 25 mm diam Ni electrodes separated by 9 mm, a saturation in threshold current at about 7.5 kA was observed for peak currents greater than 9 kA. Simultaneous anode temperature measurements indicated that the Ni anode surface temperature immediately prior to transition rose from about 1550° K to 2250° K with variations of peak current from 5 kA to 13 kA. Predictions of the variation of threshold current based on random transitions, and on cathode spot migration over the edge of the cathode, are compared with the experimental data.     

A low-threshold and high-power oxide-confined 850-nm AlInGaAs strained quantum-well vertical-cavity surface-emitting laser

A low-threshold and high-power oxide-confined 850-nm AlInGaAs strained quantum-well (QW) vertical-cavity surface-emitting laser (VCSEL) based on an intra-cavity contacted structure is fabricated. A threshold current of 1.5 mA for a 22 μm oxide aperture device is achieved, which corresponds to a threshold current density of 0.395 kA/cm². The peak output optical power reaches 17.5 mW at an injection current of 30 mA at room temperature under pulsed operation. While under continuous-wave (CW) operation, the maximum power attains 10.5 mW. Such a device demonstrates a high characteristic temperature of 327 K within a temperature range from -12℃ to 96℃ and good reliability under a lifetime test. There is almost no decrease of the optical power when the device operates at a current of 5 mA at room temperature under the CW injection current.     

Evidence for separatrix formation and sustainment with steady inductive helicity injection

The first sustainment of toroidal plasma current of 50 kA at up to 3 times the injected currents, added in quadrature, using steady inductive helicity injection is described. Separatrix currents-currents not linking the helicity injectors-are sustained up to 40 kA. Decreases in the n=1 toroidal mode of the poloidal magnetic field at higher current amplifications indicate more quiescent, direct toroidal current drive. Results are achieved in HIT-SI (with a spheromak of major radius 0.3 m) during deuterium operations immediately after helium operation. These results represent a breakthrough in the development of this new current drive method for magnetic confinement fusion.