JPH0435815Y2 - - Google Patents

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Publication number
JPH0435815Y2
JPH0435815Y2 JP17041585U JP17041585U JPH0435815Y2 JP H0435815 Y2 JPH0435815 Y2 JP H0435815Y2 JP 17041585 U JP17041585 U JP 17041585U JP 17041585 U JP17041585 U JP 17041585U JP H0435815 Y2 JPH0435815 Y2 JP H0435815Y2
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Japan
Prior art keywords
discharge
circuit
voltage
charging
high voltage
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JPS6279174U (en
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  • Tests Of Electronic Circuits (AREA)
  • Testing Or Measuring Of Semiconductors Or The Like (AREA)

Description

【考案の詳細な説明】 (産業上の利用分野) 本考案は、大規模集積回路、集積回路、半導体
素子、微細構造の電子部品又は各種電子機器等に
対して静電気放電が与える電気的オーバーストレ
ス或は電磁妨害作用若しくは上記各種電子回路、
部品及び機器等の静電気放電に対する感受性等を
試験評価するために、静電気放電を人為的に生ぜ
しめる静電気放電シミユレータに関するものであ
る。
[Detailed description of the invention] (Field of industrial application) The present invention is designed to reduce the electrical overstress caused by electrostatic discharge to large-scale integrated circuits, integrated circuits, semiconductor elements, microstructured electronic components, and various electronic devices. or electromagnetic interference or the various electronic circuits mentioned above,
This invention relates to an electrostatic discharge simulator that artificially generates electrostatic discharge in order to test and evaluate the sensitivity of parts, equipment, etc. to electrostatic discharge.

(従来の技術) 上記のような各種電子回路、部品及び機器等に
対する静電気放電は、地気から絶縁された導体よ
り成る帯電体、就中、人体の帯電電荷による静電
気放電が最も多く、したがつて、従来の静電気放
電シミユレータの多くは、帯電人体を等価的にモ
デル化したものが用いられている。
(Prior Art) The electrostatic discharges to the various electronic circuits, parts, equipment, etc. mentioned above are most often caused by electrostatic charges from charged objects made of conductors insulated from the earth, especially the human body. Therefore, many conventional electrostatic discharge simulators use equivalent models of a charged human body.

第3図は、従来の静電気放電シミユレータの一
例の要部を示す図で、SDC3は充電用直流電源、
SWSはリレースイツチ等より成る電源スイツチ、
SWDは電源スイツチSWSの開閉制御用スイツチ、
SDは電源スイツチSWSの駆動用電源、RCは充電
抵抗、CCDは充放電コンデンサ、RDは放電抵抗、
SEDは放電電極、GAPは放電間隙、EUTは被試
験体である。
Figure 3 is a diagram showing the main parts of an example of a conventional electrostatic discharge simulator, where S DC3 is a DC power supply for charging;
SW S is a power switch consisting of a relay switch, etc.
SW D is a switch for opening/closing control of power switch SW S ,
S D is the power supply for driving the power switch SW S , R C is the charging resistor, C CD is the charging/discharging capacitor, R D is the discharging resistor,
SED is the discharge electrode, GAP is the discharge gap, and EUT is the test object.

人体の帯電電圧は通常数kVから10数kVに達
し、場合によつては最高30数kVに及ぶこともあ
るので、上記従来の静電気放電シミユレータにお
いても充電用直流電源SDC3の出力電圧をOV乃至
30数kVの範囲に亙つて可変ならしめ、充放電コ
ンデンサCCDの充電電圧を各種所要値に設定し得
るように構成している。
The charging voltage of the human body normally reaches from several kV to 10-odd kV, and in some cases can reach up to 30-odd kV. Therefore, in the conventional electrostatic discharge simulator mentioned above, the output voltage of the charging DC power supply S DC3 is ~
It is configured to be variable over a range of 30-odd kV, so that the charging voltage of the charging/discharging capacitor C CD can be set to various required values.

又、充放電コンデンサCCDの静電容量及び放電
抵抗RDの抵抗値は、帯電人体の静電容量及び抵
抗と等価ならしめるが、人体の静電容量及び抵抗
の実測値は相当広い変化範囲を有し、代表値とし
て充放電コンデンサCCDの等価静電容量は50pF乃
至250pF、放電抵抗RDの等価抵抗は100Ω乃至
1500Ωの各範囲から適当な固定値を選択してい
る。
In addition, the capacitance of the charge/discharge capacitor C CD and the resistance value of the discharge resistor R D are made equivalent to the capacitance and resistance of a charged human body, but the actual values of the capacitance and resistance of the human body vary over a fairly wide range. As typical values, the equivalent capacitance of the charging/discharging capacitor C CD is 50 pF to 250 pF, and the equivalent resistance of the discharging resistor R D is 100 Ω to 250 pF.
An appropriate fixed value is selected from each range of 1500Ω.

上記従来の静電気放電シミユレータにおいて
は、充放電コンデンサCCDを予め所要電圧に充電
した後、放電電極SEDを徐々に被試験体EUTに
接近させると、放電間隙GAPの長さと気圧との
積が充放電コンデンサCCDの充電電圧に応じた値
に達した際に、放電電極SEDと被試験体EUT間
に生ずる火花放電によつて充放電コンデンサCCD
の電荷が瞬間的に被試験体EUTに加えられる。
In the above-mentioned conventional electrostatic discharge simulator, after charging the charge/discharge capacitor C CD to the required voltage, when the discharge electrode SED is gradually brought closer to the EUT under test, the product of the length of the discharge gap GAP and the atmospheric pressure increases. When the charging voltage of the discharge capacitor C CD reaches a value corresponding to the charging voltage of the discharge capacitor C CD , a spark discharge occurs between the discharge electrode SED and the EUT under test.
electric charge is instantaneously applied to the EUT under test.

(考案が解決しようとする問題点) 上記従来の静電気放電シミユレータにおいて
は、放電電極SEDを徐々に被試験体EUTに接近
させる操作が繁雑なばかりでなく、放電電極
SEDの接近の速さ及び被試験体EUTの表面の中、
放電電極SEDが正対する表面の状態に応じて放
電試験毎に放電間隙GAPの長さが異なり、した
がつて、放電試験の再現性に乏しい欠点がある。
(Problems to be solved by the invention) In the conventional electrostatic discharge simulator mentioned above, not only is the operation of gradually bringing the discharge electrode SED closer to the EUT under test, but also the discharge electrode
The approaching speed of the SED and the surface of the EUT under test,
The length of the discharge gap GAP differs for each discharge test depending on the condition of the surface directly facing the discharge electrode SED, and therefore, there is a drawback that the reproducibility of the discharge test is poor.

放電電極SEDと被試験体EUT間の放電間隙
GAPを一定に保つために静電気放電シミユレー
タを固定するときは、放電試験回数を1回乃至数
回等のように所要回数に限定して行うことが不可
能となる。即ち、電源スイツチSWSの開閉に当つ
て開閉制御用スイツチSWDの開閉から電源スイツ
チSWSの開閉までに時間の遅れを伴うのを避け得
ないため、所要回数の放電試験の終了と同時に開
閉制御用スイツチSWDを開放しても電源スイツチ
SWSの開放までの時間の遅れの間に、充放電コン
デンサCCDの充電が行われて必要以上の放電が行
われることとなる。
Discharge gap between discharge electrode SED and EUT under test
When the electrostatic discharge simulator is fixed in order to keep the GAP constant, it becomes impossible to limit the number of discharge tests to a required number of times, such as once or several times. In other words, when opening/closing the power switch SW S , it is unavoidable that there is a time delay between opening/closing the switching control switch SW D and opening/closing the power switch SW S , so the switching is performed at the same time as the required number of discharge tests are completed. Even if the control switch SW D is opened, the power switch will not turn off.
During the time delay until SW S is opened, the charge/discharge capacitor C CD is charged and discharged more than necessary.

所要回数の放電試験を正確に行うには、放電電
極SEDを被試験体EUTから遠ざけて充放電コン
デンサCCDの充電を行つた後、放電電極SEDを
徐々に被試験体EUTに接近させて放電を行い、
再び放電間隙GAPを大ならしめた状態で、充放
電コンデンサCCDを充電する操作を所要回数だけ
行うことにより目的を達し得るが、操作が極めて
繁雑なばかりでなく、前述ように放電試験の再現
性に乏しい欠点を免れることが出来ない。
To accurately perform the required number of discharge tests, move the discharge electrode SED away from the EUT under test to charge the charge/discharge capacitor C CD , then gradually bring the discharge electrode SED closer to the EUT under test to discharge. and
The purpose can be achieved by increasing the discharge gap GAP again and charging the charging/discharging capacitor C CD the required number of times, but not only is the operation extremely complicated, but it is also difficult to reproduce the discharge test as mentioned above. They cannot escape the flaws of being poor in their sexuality.

即ち、従来の静電気放電シミユレータにおいて
は、良好な再現性を以て正確に所要回数だけの放
電試験を行うことは不可能である。
That is, with conventional electrostatic discharge simulators, it is impossible to accurately conduct discharge tests the required number of times with good reproducibility.

又、電源スイツチSWSを高圧回路に挿入してい
ること第3図示の通りであるが、高圧用開閉スイ
ツチとして十分に満足し得るスイツチの実現は極
めて困難で、コスト高となるを免れ得ない。
In addition, the power switch SW S is inserted into the high voltage circuit as shown in Figure 3, but it is extremely difficult to realize a switch that is fully satisfactory as a high voltage opening/closing switch, and it is inevitable that the cost will be high. .

(問題点を解決するための手段、実施例) 本考案は、上記従来の欠点を除くためになされ
たもので、以下、図面を用いて詳細に説明する。
(Means for Solving Problems, Embodiments) The present invention has been made to eliminate the above-mentioned conventional drawbacks, and will be described in detail below with reference to the drawings.

第1図は、本考案の一実施例を示す図で、ED1
及びED2は対向電極で、各周辺部を板状に形成
し、各中心部に凹陥部(外側から見た場合には突
出部)を形成してある。RSPはリング状の誘電
体板で、電極ED1及びED2の各凹陥部に対応する
部分に孔隙を穿ち、電極ED1及びED2の間に介在
せしめて電極ED1及びED2と共に一体に形成して
ある。SED1及びSED2は放電電極で、それぞれ電
極ED1及びED2の各凹陥部に取り付けてある。
CTTは接触子で、先端を先鋭ならしめ、後端を
電極ED1の周辺部に取り付けてある。CRは放電
電流検出用の環状磁心で、絶縁体を介して接触子
CTTを取り囲むように設けてある。COLは磁心
CRに捲回したコイル、REは電圧取出用抵抗、RH
は高抵抗で、電極ED1と地気間に挿入してある。
RDは放電抵抗、CCDは充放電コンデンサ、RCは充
電抵抗、INVは直流交流変換回路で、例えば交
互に開閉せしめられる1対のスイツチング素子
(例えばサイリスタ)回路を以て構成したインバ
ータ回路等より成る。SDC1は電流電源、ANDは
開閉素子で、例えばアンドゲート回路又はスイツ
チングトランジスタ回路等より成る。OSCは直
流交流変換回路INVの駆動源で、例えば交流発
振回路より成る。Tは昇圧用変圧器、CKTは多
段倍電圧整流回路、MULはタイマで、例えばマ
ルチバイブレータより成る。SWTは切換スイツ
チ、SWMSは始動スイツチ、CEDはパルス電圧送
出回路で、例えばクロツクパルス発振回路及びフ
リツプフロツプ回路等を主たる構成素子とし、始
動スイツチSWMSの閉成時に生ずるチヤタリング
を抑え、クロツクパルス間隔を時間幅とする1個
のパルス電圧を送出するように構成した従来公知
の適宜回路より成る。LATはラツチ回路で、例
えば適当なフリツプフロツプ回路より成る。
WSDは波形整形回路、SDC2は直流電源である。
FIG. 1 is a diagram showing an embodiment of the present invention, ED 1
and ED 2 are counter electrodes, each peripheral portion of which is formed into a plate shape, and each central portion of which is formed with a concave portion (a protruding portion when viewed from the outside). RSP is a ring-shaped dielectric plate with holes formed in the parts corresponding to the recesses of electrodes ED 1 and ED 2 , and is interposed between electrodes ED 1 and ED 2 to be integrated with electrodes ED 1 and ED 2 . It has been formed. SED 1 and SED 2 are discharge electrodes, and are attached to respective recesses of electrodes ED 1 and ED 2 , respectively.
CTT is a contact with a sharp tip and a rear end attached to the periphery of electrode ED 1 . CR is a ring-shaped magnetic core for detecting discharge current, and a contact is inserted through an insulator.
It is installed to surround the CTT. COL is magnetic core
Coil wound around CR, R E is voltage extraction resistor, R H
has a high resistance and is inserted between electrode ED 1 and the ground air.
R D is a discharging resistor, C CD is a charging/discharging capacitor, R C is a charging resistor, and INV is a DC/AC conversion circuit, such as an inverter circuit configured with a pair of switching elements (such as a thyristor) circuit that are alternately opened and closed. Become. S DC1 is a current power supply, AND is a switching element, and is composed of, for example, an AND gate circuit or a switching transistor circuit. The OSC is a drive source for the DC/AC conversion circuit INV, and is composed of, for example, an AC oscillation circuit. T is a step-up transformer, CKT is a multi-stage voltage doubler rectifier circuit, and MUL is a timer, such as a multivibrator. SW T is a changeover switch, SW MS is a starting switch, and CED is a pulse voltage sending circuit. For example, the main components are a clock pulse oscillation circuit and a flip-flop circuit, etc., to suppress the chattering that occurs when the starting switch SW MS is closed, and to reduce the clock pulse interval. It consists of a conventionally known appropriate circuit configured to send out one pulse voltage having a time width. A LAT is a latch circuit, for example consisting of a suitable flip-flop circuit.
WSD is a waveform shaping circuit, and S DC2 is a DC power supply.

尚、本案静電気放電シミユレータにおいても充
放電コンデンサCCDは50pF乃至250pFの範囲から
適宜の静電容量を有するものを選択し、放電抵抗
RDは100Ω乃至1500Ωの範囲から適当な抵抗値を
有するものを選択すること従来同様で、又、直流
電源SDC1として例えば出力電圧がOV乃至24Vの
範囲で可変ならしめ得るものを用い、変圧器Tの
変圧比を適当に選ぶと共に、多段倍電圧整流回路
CKTの構成を適当ならしめることにより、充放
電コンデンサCCDをOV乃至数10kVの範囲におい
て所要の電圧に充電し得るように構成してある。
In addition, in the proposed electrostatic discharge simulator, a charge/discharge capacitor C CD with an appropriate capacitance is selected from the range of 50 pF to 250 pF, and a discharge resistor is selected.
For R In addition to appropriately selecting the transformer ratio of the transformer T, the multi-stage voltage doubler rectifier circuit
By appropriately configuring the CKT, the charging/discharging capacitor C CD can be charged to a required voltage in the range of OV to several tens of kV.

切換スイツチSWTを接点m側に切換えると共
に、接触子CTTの先端を被試験体EUTの所要個
所に接触せしめた後、始動スイツチSWMSを閉成
せしめると、パルス電圧送出回路CEDから送出
された1個のパルス電圧が切換スイツチSWTを介
してラツチ回路LATにセツト信号として加えら
れ、ラツチ回路LATの出力信号によつてアンド
ゲート回路ANDが導通する。
After switching the changeover switch SW T to the contact m side and bringing the tip of the contactor CTT into contact with the required location on the EUT under test, the start switch SW MS is closed, and the pulse voltage is sent from the pulse voltage sending circuit CED. One pulse voltage is applied as a set signal to the latch circuit LAT via the changeover switch SW T , and the AND gate circuit AND is made conductive by the output signal of the latch circuit LAT.

アンドゲート回路ANDの導通に応じて交流発
振回路OSCの発振出力がアンドゲート回路AND
を介して直流交流変換回路INVを形成するイン
バータに加えられ、直流電源SDC1から加えられる
直流電圧を交流電圧に変換する。
In response to the conduction of the AND gate circuit AND, the oscillation output of the AC oscillation circuit OSC changes to the AND gate circuit AND.
It is applied to the inverter forming the DC/AC converter circuit INV via the DC power supply S DC1, and converts the DC voltage applied from the DC power supply S DC1 into AC voltage.

この変換交流電圧は変圧器Tを介して多段倍電
圧整流回路CKTに加えられ、その出力直流高電
圧は充電抵抗RCを介して充放電コンデンサCCD
充電する。充放電コンデンサCCDの充電電圧が放
電電極SED1及びSED2間における放電間隙の長さ
に対応した電圧に達すると、放電間隙に火花放電
を生じ、充放電コンデンサCCDの電荷が瞬間的に
被試験体EUTに加えられる。
This converted AC voltage is applied to a multi-stage voltage doubler rectifier circuit CKT via a transformer T, and the output DC high voltage charges a charge/discharge capacitor C CD via a charging resistor R C . When the charging voltage of the charge/discharge capacitor C CD reaches a voltage corresponding to the length of the discharge gap between the discharge electrodes SED 1 and SED 2 , a spark discharge occurs in the discharge gap, and the charge of the charge/discharge capacitor C CD is instantaneously reduced. Added to EUT under test.

被試験体EUTに放電電極が加えられると、接
触子CTTの周りに設けた磁心CRを介してコイル
COLに誘起したパルス電流によつて、電圧取出
用抵抗REに生じた電圧降下が波形整形回路WSC
において一定時間幅のパルス電圧に整形された
後、ラツチ回路LATにリセツト信号として加え
られ、ラツチ回路LATの出力電圧を消滅せしめ
る。ラツチ回路LATの出力電圧の消滅に応じて
アンドゲート回路ANDが遮断し、充放電コンデ
ンサCCDの充電が停止される。
When a discharge electrode is added to the EUT under test, the coil is connected via the magnetic core CR provided around the contactor CTT.
The voltage drop that occurs in the voltage extraction resistor R E due to the pulse current induced in COL causes the waveform shaping circuit WSC
After being shaped into a pulse voltage with a constant time width, it is applied as a reset signal to the latch circuit LAT, causing the output voltage of the latch circuit LAT to disappear. When the output voltage of the latch circuit LAT disappears, the AND gate circuit AND is cut off, and charging of the charge/discharge capacitor C CD is stopped.

始動スイツチSWMSを開放した後、再び閉成す
ると、前記と同様にして放電が行われる。即ち、
始動スイツチSWMSを1回閉成する毎に1回ずつ
放電試験を行うことが出来る。
When the starting switch SW MS is opened and then closed again, discharge occurs in the same manner as described above. That is,
A discharge test can be performed once each time the starting switch SW MS is closed.

第2図は、以上の動作を説明するためのタイム
チヤートで、Aは始動スイツチSWMSの開閉状態、
Bはパルス送出回路CEDから送出されるパルス
電圧、Cはラツチ回路LATの出力電圧、Dは多
段倍電圧整流回路CKTの出力電圧、Eは充放電
コンデンサCCDの充電電圧、Fは磁心CR、コイル
COL及び抵抗REを介して取り出された放電検出
電圧、Gは波形整形回路WSCの出力電圧の各波
形図である。
Figure 2 is a time chart to explain the above operation, where A is the open/closed state of the start switch SW MS ;
B is the pulse voltage sent from the pulse sending circuit CED, C is the output voltage of the latch circuit LAT, D is the output voltage of the multi-stage voltage doubler rectifier circuit CKT, E is the charging voltage of the charging/discharging capacitor C CD , F is the magnetic core CR, coil
The discharge detection voltage taken out via COL and the resistor RE , and G are each waveform diagram of the output voltage of the waveform shaping circuit WSC.

次に、切換スイツチSWTを接点a側に切換えて
マルチバイブレータMULを始動せしめると、そ
の発振出力(第2図H)がラツチ回路LATに加
えられ、その出力(第2図C′)によりアンドゲー
ト回路ANDが導通し、前記と同様にして放電試
験が行われ、放電検出パルス電圧(第2図F′)の
波形整形電圧(第2図G′)がラツチ回路LATに
加えられると、ラツチ回路LATの出力C′が消滅
し、アンドゲート回路ANDが遮断して充放電コ
ンデンサCCDの充電が停止される。マルチバイブ
レータMULからの次の出力電圧Hがラツチ回路
LATに加えられると、ラツチ回路LATが再び出
力を送出し、アンドゲート回路ANDが導通して
充放電コンデンサCCDの充電が再開され、以下、
前記と同様の繰り返しによつて放電試験が反覆し
て行われる。尚、第2図D′及びE′は、この場合に
おける多段倍電圧整流回路CKTの出力電圧及び
充放電コンデンサCCDの充電電圧の各波形図であ
る。
Next, when the changeover switch SW T is switched to contact a side to start the multivibrator MUL, its oscillation output (H in Fig. 2) is applied to the latch circuit LAT, and its output (C' in Fig. 2) When the gate circuit AND becomes conductive and a discharge test is performed in the same manner as above, the waveform shaping voltage (G' in Figure 2) of the discharge detection pulse voltage (F' in Figure 2) is applied to the latch circuit LAT. The output C' of the circuit LAT disappears, the AND gate circuit AND is cut off, and charging of the charging/discharging capacitor C CD is stopped. The next output voltage H from the multivibrator MUL is a latch circuit.
When applied to LAT, the latch circuit LAT sends out an output again, the AND gate circuit AND conducts, and charging of the charging/discharging capacitor C CD is resumed, as follows:
The discharge test is repeated in the same manner as above. Incidentally, FIGS. 2D' and E' are waveform diagrams of the output voltage of the multistage voltage doubler rectifier circuit CKT and the charging voltage of the charge/discharge capacitor C CD in this case.

切換スイツチSWT接点a側に切換えてマルチバ
イブレータMULの発振出力をラツチ回路LATに
加えた場合には、マルチバイブレータMULの発
振周期が充放電コンデンサCCDの充電回路におけ
る時定数より長ければ、放電の繰返周期はマルチ
バイブレータMULの発振周期によつて定まるこ
ととなる。
When the changeover switch SW T contact is switched to the a side and the oscillation output of the multivibrator MUL is applied to the latch circuit LAT, if the oscillation period of the multivibrator MUL is longer than the time constant in the charging circuit of the charge/discharge capacitor C CD , the discharge will start. The repetition period of is determined by the oscillation period of the multivibrator MUL.

第1図には、直流交流変換回路INVを他励形
回路を以て形成した場合を例示したが、自励形回
路を以て形成してもよく、直流交流変換回路
INVによつて直流電源SDC1の電圧を交流電圧に変
換する代りに、例えば商用交流電圧を開閉素子を
介して多段倍電圧整流回路CKTに加えるように
構成するか、直流電源SDC1、直流交流変換回路
INV、交流発振回路OSC、アンドゲート回路
AND、変圧器T及び多段倍電圧整流回路CKTを
以て直流高電圧源を構成する代りに、例えばフラ
イバツク直流高電圧源の出力電圧を、例えば、所
謂サイリスタ、高圧用トランジスタ、モス形電界
効果トランジスタ等の高圧用半導体スイツチング
素子を介して充放電コンデンサCCDに加えると共
に、高圧用半導体スイツチング素子の開閉をラツ
チ回路LATの出力によつて制御するように構成
してもよい。
Although FIG. 1 shows an example in which the DC/AC converter circuit INV is formed using a separately excited type circuit, it may also be formed using a self-excited type circuit.
Instead of converting the voltage of the DC power supply S DC1 into an AC voltage by INV, for example, the commercial AC voltage can be configured to be applied to the multi-stage voltage doubler rectifier circuit CKT via a switching element, or the DC power supply S DC1 , DC AC conversion circuit
INV, AC oscillation circuit OSC, AND gate circuit
Instead of configuring a DC high voltage source using an AND, a transformer T, and a multi-stage voltage doubler rectifier circuit CKT, for example, the output voltage of a flyback DC high voltage source can be changed to a so-called thyristor, high voltage transistor, MOS type field effect transistor, etc. It may be configured such that it is applied to the charge/discharge capacitor C CD via a high voltage semiconductor switching element, and the opening/closing of the high voltage semiconductor switching element is controlled by the output of the latch circuit LAT.

又、磁心CR、コイルCOL及び抵抗REによつて
放電を検出する代りに、第1図に点線を以て示す
ように、導体板CDを誘電体板IPを介して電極
ED2と対向せしめ、導体板CDと電極ED2間の容
量及び電圧取出用抵抗R′Eを介して放電検出電圧
を取り出すように形成しても本考案を実施し得る
こと勿論である。
Also, instead of detecting the discharge using the magnetic core CR, coil COL, and resistor RE , as shown by the dotted line in Figure 1, the conductor plate CD is connected to the electrode via the dielectric plate IP.
Of course, the present invention can also be implemented by forming the electrode ED 2 to face the electrode ED 2 so as to take out the discharge detection voltage through the capacitance between the conductor plate CD and the electrode ED 2 and the voltage take-out resistor R'E.

(考案の効果) 本案静電気放電シミユレータにおいては、放電
電極SED1及びSED2間における放電間隙の長さを
一定に保持し得ると共に、最初から接触子CTT
を被試験体EUTに接触せしめたままの状態で放
電試験を行い得るように構成してあるから、放電
電極を被試験体に徐々に接近させて放電試験を行
う静電気放電シミユレータに較べて取扱いが遥か
に容易となると共に、放電間隙の長さを正確に一
定に保つて放電を行い得るから再現性の良好な放
電試験の実施が可能で、更に、切換スイツチング
SWTを接点m側に切換えて始動スイツチSWMS
閉成することにより1回限りの放電試験を実施す
ることが出来、始動スイツチSWMSを間欠的に繰
返し閉成することにより、放電試験を任意所要回
数だけ正確に行うことが可能なると共に、切換ス
イツチSWT及び始動スイツチSWMSの挿入個所は
低圧回路部分であるから、両スイツチ共に特別の
高圧用高速スイツチを用いなくとも回路の切換え
及び開閉を迅速に行い得ると共に、取扱いに危険
を伴うおそれもない。
(Effect of the invention) In the electrostatic discharge simulator of the present invention, the length of the discharge gap between the discharge electrodes SED 1 and SED 2 can be kept constant, and the contactor CTT
Because it is configured so that a discharge test can be performed while the EUT remains in contact with the EUT under test, it is easier to handle than an electrostatic discharge simulator, which performs a discharge test by gradually bringing the discharge electrode closer to the EUT under test. In addition to being much easier, it is possible to carry out discharge while maintaining the length of the discharge gap accurately, making it possible to conduct discharge tests with good reproducibility.
A one-time discharge test can be performed by switching SW T to the contact m side and closing the starting switch SW MS.A discharge test can be performed by repeatedly closing the starting switch SW MS intermittently. In addition to being able to accurately perform the desired number of operations, the changeover switch SW T and starting switch SW MS are inserted into the low voltage circuit, so both switches can be switched and switched without using a special high-speed switch for high voltage. It can be opened and closed quickly and there is no danger of handling it.

尚、第1図には、放電電極SED1及びSED2の他
に対向電極ED1及びED2を設けた場合を例示した
が、電極ED1及びED2を省いても本考案を実施す
ることが出来る。
Although FIG. 1 shows an example in which the counter electrodes ED 1 and ED 2 are provided in addition to the discharge electrodes SED 1 and SED 2 , the present invention can be carried out even if the electrodes ED 1 and ED 2 are omitted. I can do it.

然しながら、対向電極ED1及びED2を設けた場
合には、次のような効果を生ぜしめることが出来
る。
However, when the counter electrodes ED 1 and ED 2 are provided, the following effects can be produced.

即ち、対向電極ED1及びED2を設けていない場
合には、放電電極SED1及びSED2間に充放電コン
デンサCCDの電荷が供給されると、その初期にお
いて火花空間の導電率が上昇し、その上昇過程に
おいて充放電コンデンサCCDの電荷の一部が火花
空間において失われ、その結果、火花放電の生成
過程における火花空間の電界強度が低下し、この
電界強度の低下によつて導電率の上昇作用が弱め
られ、本来の上昇時間に対応する軌跡に沿つての
導電率の上昇が行われなくなり、放電電流の立上
り時間が放電間隙の長さ及び気圧に依存して定ま
る一定時間に比し著しく遅れ、その結果、放電電
流の波形に歪を生じ、放電試験の評価の信頼性を
低下せしめるおそれがある。
That is, when the counter electrodes ED 1 and ED 2 are not provided, when the charge of the charging/discharging capacitor C CD is supplied between the discharge electrodes SED 1 and SED 2 , the conductivity of the spark space increases at the initial stage. , in the rising process, a part of the charge of the charging/discharging capacitor C CD is lost in the spark space, and as a result, the electric field strength in the spark space during the spark discharge generation process decreases, and this decrease in electric field strength causes the conductivity to decrease. The increasing effect of the increase in conductivity is weakened, the conductivity does not increase along the trajectory corresponding to the original rise time, and the rise time of the discharge current is compared to a constant time determined depending on the length of the discharge gap and the atmospheric pressure. As a result, the waveform of the discharge current may be distorted, which may reduce the reliability of the evaluation of the discharge test.

これに対して対向電極ED1及びED2を設けた場
合には、充放電コンデンサCCDの充電に際して対
向電極ED1及びED2間に形成される容量も亦高抵
抗RHを介して充電される。
On the other hand, when the opposing electrodes ED 1 and ED 2 are provided, the capacitance formed between the opposing electrodes ED 1 and ED 2 when charging the charging/discharging capacitor C CD is also charged via the high resistance R H. Ru.

そして放電電極SED1及びSED2間の放電間隙に
おける火花放電開始の初期において、充放電コン
デンサCCDの電荷が放電抵抗RDを介して火花空間
に注入されようとするが、放電抵抗RD及び放電
間隙における火花抵抗により制限されて火花空間
に注入される電荷量は極めて僅かとなる。
At the beginning of the spark discharge in the discharge gap between the discharge electrodes SED 1 and SED 2 , the charge of the charging/discharging capacitor C CD is about to be injected into the spark space via the discharge resistor R D , but the discharge resistor R D and Limited by the spark resistance in the discharge gap, the amount of charge injected into the spark space is extremely small.

然しながら、対向電極ED1及びED2間の容量は
放電間隙に並列に接続されており、対向電極ED1
及びED2間の電荷は、放電抵抗に関係なく放電間
隙における火花抵抗にのみ制限されて火花空間に
注入されるから、対向電極ED1及びED2により形
成される並列容量から火花空間に注入される電荷
量は、充放電コンデンサCCDから注入される電荷
量に比し極めて大となり、放電間隙における導電
率の増大に伴つて並列容量の電荷の全てが火花空
間にのみ注入されることとなる。
However, the capacitance between the counter electrodes ED 1 and ED 2 is connected in parallel to the discharge gap, and the capacitance between the counter electrodes ED 1 and ED 2 is
Since the charge between ED 2 and ED 2 is limited only by the spark resistance in the discharge gap regardless of the discharge resistance and is injected into the spark space, it is injected into the spark space from the parallel capacitance formed by the opposing electrodes ED 1 and ED 2 . The amount of charge that is injected from the charge/discharge capacitor C CD is extremely large compared to the amount of charge injected from the charge/discharge capacitor C CD, and as the conductivity increases in the discharge gap, all of the charge in the parallel capacitance is injected only into the spark space. .

したがつて、対向電極ED1及びED2により形成
される並列容量を適宜大ならしめると共に、この
並列容量と放電間隙とを結ぶ電流径路のインピー
ダンスを出来るだけ小ならしめておけば、並列容
量から火花空間への電荷の注入は極めて速やかに
行われ、充放電コンデンサCCDの電荷を殆ど失う
ことなく放電間隙を閃絡せしめて、充放電コンデ
ンサCCDの電荷の殆ど全てを被試験体EUTに加え
得ると共に、放電電流の波形を理想波形に極めて
近い波形となし、放電試験の信頼性を高めること
が出来る。
Therefore, if the parallel capacitance formed by the opposing electrodes ED 1 and ED 2 is increased appropriately and the impedance of the current path connecting this parallel capacitance and the discharge gap is made as small as possible, sparks can be prevented from the parallel capacitance. The charge is injected into the space extremely quickly, causing the discharge gap to flash over without losing much of the charge on the charge/discharge capacitor C CD , and almost all of the charge on the charge/discharge capacitor C CD is added to the EUT under test. At the same time, the waveform of the discharge current can be made extremely close to the ideal waveform, and the reliability of the discharge test can be improved.

この場合、被試験体EUTに加えられるエネル
ギは、充放電コンデンサCCDから放電間隙を介し
て放出される電流によつてのみ定まり、並列容量
の電荷には無関係である。
In this case, the energy applied to the EUT under test is determined only by the current discharged from the charge/discharge capacitor C CD via the discharge gap and is independent of the charge of the parallel capacitor.

又、電極ED1と地気間に挿入された抵抗RHの値
を被試験体EUTのインピーダンスに比し十分高
く選んでおけば、放電電流が抵抗RHに分流する
おそれはない。
Furthermore, if the value of the resistor R H inserted between the electrode ED 1 and the ground air is selected to be sufficiently high compared to the impedance of the EUT under test, there is no possibility that the discharge current will be shunted to the resistor R H.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は、本考案の一実施例を示す図、第2図
は、その作動説明のためのタイムチヤート、第3
図は、従来の静電気放電シミユレータの要部を示
す図で、ED1及びED2……対向電極、RSPリング
状誘電体板、SED1,SED2及びSED……放電電
極、CTT……接触子、CR……環状磁心、COL…
…コイル、RE及びR′E……電圧取出用抵抗、RH
…高抵抗、RD……放電抵抗、CCD……充放電コン
デンサ、RC……充電抵抗、INV……直流交流変
換回路、SDC1,SDC2,SDC3及びSD……直流電源、
AND……開閉回路、OSC……駆動源、T……変
圧器、CKT……多段倍電圧整流回路、MUL……
タイマ、SWT,SWMS,SWS及びSWD……スイツ
チ、CED……パルス電圧送出回路、LAT……ラ
ツチ回路、WSC……波形整形回路、GAP……放
電間隙、EUT……被試験体、CD……導体板、IP
……誘電体板である。
Fig. 1 is a diagram showing an embodiment of the present invention, Fig. 2 is a time chart for explaining its operation, and Fig. 3 is a diagram showing an embodiment of the present invention.
The figure shows the main parts of a conventional electrostatic discharge simulator. ED 1 and ED 2 ... counter electrode, RSP ring-shaped dielectric plate, SED 1 , SED 2 and SED ... discharge electrode, CTT ... contactor. , CR...Annular magnetic core, COL...
...Coil, R E and R′ E ...Resistance for voltage extraction, R H ...
...High resistance, R D ...Discharging resistance, C CD ...Charging and discharging capacitor, R C ...Charging resistance, INV ...DC AC conversion circuit, S DC1 , S DC2 , S DC3 and S D ...DC power supply,
AND...Switching circuit, OSC...Drive source, T...Transformer, CKT...Multi-stage voltage doubler rectifier circuit, MUL...
Timer, SW T , SW MS , SW S and SW D ... Switch, CED ... Pulse voltage sending circuit, LAT ... Latch circuit, WSC ... Waveform shaping circuit, GAP ... Discharge gap, EUT ... Test object , CD...conductor plate, IP
...It is a dielectric plate.

Claims (1)

【実用新案登録請求の範囲】 (1) 充放電コンデンサの電荷を被試験体に加える
ための放電抵抗及び放電電極と、充電抵抗を介
して前記充放電コンデンサに直流電圧を加える
直流高電圧源と、タイマから送出される周期的
パルス電圧又は手動開閉スイツチの閉成に応じ
て形成送出されるパルス電圧を選択し、セツト
信号としてラツチ回路に加える切換スイツチ
と、前記充放電コンデンサの放電電流を検出
し、リセツト信号として前記ラツチ回路に加え
る放電電流検出素子と、前記ラツチ回路の出力
を、前記直流高電圧源の出力を開閉する開閉素
子の開閉制御信号として加える回路とより成る
ことを特徴とする静電気放電シミユレータ。 (2) 直流高電圧源が、直流電源と、その出力電圧
の加えられる直流交流変換回路と、その変換出
力の加えられる多段倍電圧整流回路とより成る
実用新案登録請求の範囲第1項記載の静電気放
電シミユレータ。 (3) 直流高電圧源が、商用交流電源等の出力電圧
の加えられる多段倍電圧整流回路より成る実用
新案登録請求の範囲第1項記載の静電気放電シ
ミユレータ。 (4) 直流高電圧源が、フライバツク直流高電圧源
より成る実用新案登録請求の範囲第1項記載の
静電気放電シミユレータ。 (5) 放電電流検出素子が電磁誘導形検出素子より
成る実用新案登録請求の範囲第1項記載の静電
気放電シミユレータ。 (6) 放電電流検出素子が静電誘導形検出素子より
成る実用新案登録請求の範囲第1項記載の静電
気放電シミユレータ。
[Claims for Utility Model Registration] (1) A discharge resistor and a discharge electrode for applying the electric charge of a charging/discharging capacitor to a test object, and a DC high voltage source for applying a DC voltage to the charging/discharging capacitor via the charging resistor. , selects the periodic pulse voltage sent from the timer or the pulse voltage formed and sent in response to the closing of the manual on/off switch, and applies the changeover switch to the latch circuit as a set signal, and detects the discharge current of the charge/discharge capacitor. and a circuit that applies the output of the latch circuit as an opening/closing control signal for a switching element that opens and closes the output of the DC high voltage source. Electrostatic discharge simulator. (2) The utility model registration claim 1, wherein the DC high voltage source comprises a DC power supply, a DC/AC conversion circuit to which its output voltage is applied, and a multistage voltage doubler rectifier circuit to which its converted output is applied. Electrostatic discharge simulator. (3) The electrostatic discharge simulator according to claim 1, wherein the DC high voltage source is a multi-stage voltage doubler rectifier circuit to which the output voltage of a commercial AC power source or the like is applied. (4) The electrostatic discharge simulator according to claim 1, wherein the DC high voltage source is a flyback DC high voltage source. (5) The electrostatic discharge simulator according to claim 1, wherein the discharge current detection element is an electromagnetic induction type detection element. (6) The electrostatic discharge simulator according to claim 1, wherein the discharge current detection element is an electrostatic induction type detection element.
JP17041585U 1985-11-07 1985-11-07 Expired JPH0435815Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17041585U JPH0435815Y2 (en) 1985-11-07 1985-11-07

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17041585U JPH0435815Y2 (en) 1985-11-07 1985-11-07

Publications (2)

Publication Number Publication Date
JPS6279174U JPS6279174U (en) 1987-05-20
JPH0435815Y2 true JPH0435815Y2 (en) 1992-08-25

Family

ID=31105124

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17041585U Expired JPH0435815Y2 (en) 1985-11-07 1985-11-07

Country Status (1)

Country Link
JP (1) JPH0435815Y2 (en)

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2020021713A1 (en) 2018-07-27 2020-01-30 パナソニック インテレクチュアル プロパティ コーポレーション オブ アメリカ Fraud detection method and electronic control device for detecting frauds

Also Published As

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