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Apparatus for measuring the reverse recovery charge of fast semiconductor diodes

机译:测量快速半导体二极管反向恢复电荷的装置

摘要

1,083,526. Measuring diode recovery charge. V#YZKUMN#Y …STAV MATEMATICK#YCH STROJ…. Jan. 13, 1966 [Jan. 28, 1965], No. 1639/66. Heading G1U. In an apparatus for measuring the reverse recovery charge of a fast semi-conductor diode, the diode D is pulsed from a generator G and the voltage produced across a load resistor R is applied to an input 5 of a sampling oscilloscope 1 having a CRT display 2. The sampling oscilloscope effects a time transposition of the reverse recovery waveform to enable it to be displayed. The charge flowing in the reverse recovery process is measured by developing a voltage which is applied to a calibration input of the sampling oscilloscope in such a manner as to shift the level of the display showing the reverse recovery so that it is equally balanced about the zero axis. The system operates in a self balancing manner to keep this calibration voltage at a value appropriate to maintain the balance, and this value is proportional to the charge to be measured. To derive this voltage, the reverse recovery waveform, applied via the sampling oscilloscope to the vertical plate 4 of the CRT, is also applied via a condenser 10 to a detector 11, 12. As the waveform swings negative into the reverse recovery region, the detector passes a pulse which triggers a gating pulse generator 13. This generator provides a pulse, whose width is adjustable, which is supplied to open the gates 14, 15. The reverse recovery waveform itself is passed via the gate 14 to the integrating network 16, 17, and the integrated signal is passed via a high gain amplifier 18 to a meter 19 and to the other input of the gate 15. The voltage is therefore passed for the period allowed by the generator 13 to the calibrating input 6 of the sampling oscilloscope. The generator 13 is set to provide a pulse slightly longer than the time required for the recovery process to be completed. Near the end of each time base sweep provided from the sampling oscilloscope a trigger signal is derived at the output 7 which operates a switch 9 via a switching pulse generator 8 to discharge the capacitor 10. The system establishes a balance such that the indicator 19 shows a voltage proportional to the recovery charge to be measured.
机译:1,083,526。测量二极管恢复电荷。 V#YZKUMN#Y…STAM MATEMATICK#YCH STROJ…。 1966年1月13日[ [1965年1月28日],第1639/66号。标题G1U。在用于测量快速半导体二极管的反向恢复电荷的设备中,二极管D从发生器G发出脉冲,并且负载电阻R两端产生的电压被施加到具有CRT显示屏的采样示波器1的输入5上。 2.采样示波器对反向恢复波形进行时间转换,使其能够显示。反向恢复过程中流动的电荷是通过产生一个电压而测量的,该电压施加到采样示波器的校准输入端上,其方式是移动显示反向恢复的显示屏的电平,以使其在零附近保持平衡。轴。系统以自平衡方式运行,以将校准电压保持在适合于保持平衡的值,并且该值与要测量的电荷成比例。为了获得该电压,还将通过采样示波器施加到CRT垂直板4的反向恢复波形通过电容器10施加到检测器11、12。当波形向负向恢复区域摆动时,检测器通过一个脉冲,该脉冲触发选通脉冲发生器13。该发生器提供一个宽度可调的脉冲,该脉冲被提供以打开门14、15。反向恢复波形本身通过门14传递到积分网络16 ,如图17所示,积分信号通过高增益放大器18到达仪表19和门15的另一个输入端。因此,电压在发生器13允许的时间内传递到采样的校准输入端6。示波器。发生器13被设置为提供比完成恢复过程所需的时间稍长的脉冲。在采样示波器提供的每个时基扫描即将结束时,在输出7处都会触发信号,该输出信号会通过开关脉冲发生器8来操作开关9以使电容器10放电。系统建立平衡,使指示器19显示与要测量的恢复电荷成比例的电压。

著录项

  • 公开/公告号GB1083526A

    专利类型

  • 公开/公告日1967-09-13

    原文格式PDF

  • 申请/专利权人 VYZKUMNY USTAV MATEMATICKYCH STROJU;

    申请/专利号GB19660001639

  • 发明设计人 HORNAK TOMAS;

    申请日1966-01-13

  • 分类号G01R31/26;

  • 国家 GB

  • 入库时间 2022-08-23 13:52:26

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