(1) Hole particle current from E to B (2)Electron particle current from B to E (3)Recombination current in B (4) Hole particle current originating in E and reaching C (5)Reverse electron particle current from c to B (6) Reverse hole particle current from b to c (What is difference between \current\ and\particle current ? OE F Schubert, Rensselaer Polytechnic Institute, 2003

10.1晶闸管的结构和工作原理 10.2单相可控整流电路 10.3晶闸管的触发电路 10.4晶闸管的保护 10.5双向晶闸管简介 10.6晶闸管应用实例

6.1 非正弦周期信号及分解 6.2 非正弦周期信号的频谱 6.3 非正弦周期信号的有效值、 平均值和平均功率 6.4 非正弦周期电路的计算

The IPMTS.OAT1/T3 Series is designed to protect voltage sensitive components from high voltage, high energy transients http:/lonsemi.com Excellent clamping capability, high surge capability, low zener impedance and fast response time. The advanced packaging technique provides for a highly efficient micro miniature, space PLASTIC SURFACE MOUNT saving surface mount with its unique heat sink design. The

Schottky Power Rectifier employing the Schottky Barrier principle in a large area metal-to-silicon power diode. State-of-the-art geometry features oN Semiconductor epitaxial construction with oxide passivation and metal overlay contact. Ideally suited for low voltage, high frequency rectification, or http:/lonsemi.com

High power diode laser ROFIN DI Series ROFIN DL X75 750 w ROFIN DL 010 000 W ROFIN DL 015 500 W ROFIN DL 020 2000 w ROFIN DL 025 2500 W ROFIN DL 030 3000 w ROFINI SINAR

已知发电机的端电压、负载电流和功率因数及 参数ra、小q 1、已知内功率因数角ψ 按照电势方程式的关系作出相量图 2、未知内功率因数角ψ 1)利用方程式求出:压l i 2)利用公式求出: arctan aitEap

4.1叠加定理 4.2替代定理 4.3戴维宁定理和诺顿定理 4.4最大功率传输定理 4.5*特勒根定理 4.6*互易定理 4.7*对偶原理

当得到代码形式的状态表后,只要选定确定电路状态的触发器的类型,就可导出各触发器的激励函数和电路的输出函数,将其电路实现便得到时序电路的逻辑图。如首先得到的是符号形式的状态表,需将其进行状态分配,得到符号形式的状态表。 一、确定激励函数(Excitation Function) 二、确定输出函数(Output Function)

本课件制作的软件平台基于是“Windows操作系统+PowerPoint2000+ Flash MX”,因此它的运行环境是也应该与之相同或至少类似,否则,将导致所作动 画部分功能无法实现和演示文稿不能正常播放因此在运行前应该确保系统可 以满足要求