JPH0435817Y2 - - Google Patents
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- Publication number
- JPH0435817Y2 JPH0435817Y2 JP17041785U JP17041785U JPH0435817Y2 JP H0435817 Y2 JPH0435817 Y2 JP H0435817Y2 JP 17041785 U JP17041785 U JP 17041785U JP 17041785 U JP17041785 U JP 17041785U JP H0435817 Y2 JPH0435817 Y2 JP H0435817Y2
- Authority
- JP
- Japan
- Prior art keywords
- discharge
- electrode
- bed
- counter electrode
- gap
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
- 239000003990 capacitor Substances 0.000 claims description 30
- 238000007599 discharging Methods 0.000 claims description 20
- 230000002093 peripheral effect Effects 0.000 claims description 9
- 239000004020 conductor Substances 0.000 claims description 6
- 239000012212 insulator Substances 0.000 claims 1
- 239000013256 coordination polymer Substances 0.000 description 7
- 238000010586 diagram Methods 0.000 description 4
- 238000009413 insulation Methods 0.000 description 4
- 239000000463 material Substances 0.000 description 3
- 230000007423 decrease Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000005684 electric field Effects 0.000 description 2
- 238000002474 experimental method Methods 0.000 description 2
- WABPQHHGFIMREM-UHFFFAOYSA-N lead(0) Chemical compound [Pb] WABPQHHGFIMREM-UHFFFAOYSA-N 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 239000000853 adhesive Substances 0.000 description 1
- 230000001070 adhesive effect Effects 0.000 description 1
- 230000004323 axial length Effects 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 230000000630 rising effect Effects 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 229920003002 synthetic resin Polymers 0.000 description 1
- 239000000057 synthetic resin Substances 0.000 description 1
Landscapes
- Tests Of Electronic Circuits (AREA)
- Elimination Of Static Electricity (AREA)
- Testing Of Individual Semiconductor Devices (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
ス又は電磁妨害作用或は上記のような各種回路、
部品、各種電子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 various circuits as mentioned above,
This invention relates to an electrostatic discharge simulator that artificially generates electrostatic discharge in order to test and evaluate the susceptibility of parts, various electronic devices, etc. to electrostatic discharge.
(従来の技術)
上記のような各種電子回路、部品、各種電子機
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、静電気放
電シミユレータの多くは、帯電した人体を等価的
にモデル化したものが用いられている。(Prior Art) The electrostatic discharges to various electronic circuits, parts, various electronic devices, etc. mentioned above are most often caused by electrostatic charges on charged objects made of conductors insulated from the earth, especially the human body. Therefore, many electrostatic discharge simulators use equivalent models of a charged human body.
第2図は、従来の静電気放電シミユレータの一
例を示す要部回路図で、CCDは帯電した人体の静
電容量と等価の静電容量を有する充放電コンデン
サ、RDは帯電した人体の抵抗と等価の抵抗値を
有する放電抵抗、SEDは放電電極、GAPは放電
間隙、EUTは被試験体である。 Figure 2 is a circuit diagram of the main parts of an example of a conventional electrostatic discharge simulator, where C CD is a charging/discharging capacitor with a capacitance equivalent to that of a charged human body, and R D is the resistance of a charged human body. 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から最高30数kVに
及ぶこともあるので、充放電コンデンサCCDの充
電電圧をOV乃至30数kVの範囲に亙つて設定し
得るように充電電源回路(図示していない)を構
成し、充放電コンデンサCCDの等価静電容量及び
放電抵抗RDの等価抵抗も亦人体の実測値に応じ
て定めるが、何れの値も相当広い変化範囲を有す
るので、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。 The charging voltage of the human body usually ranges from several kV to a maximum of 30-odd kV, so a charging power supply circuit (not shown) is designed so that the charging voltage of the charging/discharging capacitor C CD can be set in the range of OV to 30-odd kV. The equivalent capacitance of the charging/discharging capacitor C CD and the equivalent resistance of the discharging resistor R D are also determined according to the actual measured values of the human body, but since each value has a fairly wide range of variation, the representative Appropriate fixed values are selected from a range of 50 pF to 250 pF for the equivalent capacitance of the charging/discharging capacitor C CD and 100 Ω to 1500 Ω for the equivalent resistance of the discharging resistor R D.
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。 After charging the charging/discharging capacitor C CD in advance to the required voltage, when the discharging electrode SED is gradually brought closer to the EUT under test, the product of the length of the discharging gap GAP and the atmospheric pressure changes according to the charging voltage of the charging/discharging capacitor C CD . The spark discharge that occurs when this value is reached causes the electric charge of the charging/discharging capacitor C CD to be instantaneously applied to the EUT under test.
(考案が解決しようとする問題点)
静電気放電電流の波形は、原理的には指数関数
曲線に一致するが、放電工学上の火花放電現象特
有の原因によつて実際の放電電流の波形は、原理
的波形とは可成り異なつた波形となる。(Problem to be solved by the invention) In principle, the waveform of an electrostatic discharge current corresponds to an exponential curve, but due to causes specific to the spark discharge phenomenon in electrical discharge engineering, the actual waveform of the discharge current is The resulting waveform is quite different from the original waveform.
このような波形の変化は、充放電コンデンサ
CCDの電圧、即ち、放電間隙GAPにおける放電開
始電圧の変化に依存することが従来から知られて
いたが、本考案者が静電気放電シミユレータによ
る放電実験を繰り返し行つて検討した結果、次の
ような原因によつても波形変化を生ずることを明
らかにすることが出来た。 This kind of waveform change is due to the charging/discharging capacitor.
It has long been known that the voltage of C CD depends on the change in the discharge starting voltage in the discharge gap GAP, but as a result of repeated discharge experiments using an electrostatic discharge simulator, the inventor of the present invention found the following. We were able to clarify that waveform changes occur due to various causes.
即ち、放電間隙GAP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、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GAP
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、放電試験の信頼性を低下せしめることとな
る。 That is, when the electric charge of the charging/discharging capacitor C CD is supplied to the discharge gap GAP, the conductivity of the spark space increases in the initial stage, and in the rising process, a part of the electric charge of the charging/discharging capacitor C CD is lost in the spark space. The electric field strength in the spark space during the spark discharge generation process decreases, and this decrease in electric field strength weakens the effect of increasing conductivity, causing the conductivity to increase along a trajectory corresponding to the original rise time. The rise time of the discharge current is no longer carried out, and the discharge gap GAP
As a result, the waveform of the discharge current is distorted, reducing the reliability of the discharge test.
(問題点を解決するための手段及び作用)
第2図に示した静電気放電シミユレータの放電
電極SEDと、被試験体EUTの一部によつて形成
される放電電極との間における放電間隙GAPに
は、放電電極の表面積及び放電間隙GAPの長さ
に応じて1pF乃至数pF程度の浮遊容量が存在し、
火花放電生成の初期において、浮遊容量の電荷は
火花空間において速やかに消滅するので浮遊容量
の存在を殆ど無視し得るが、浮遊容量の大きさを
意図的に増大させると、次のような作動が行われ
る筈である。(Means and actions for solving the problem) In the discharge gap GAP between the discharge electrode SED of the electrostatic discharge simulator shown in Fig. 2 and the discharge electrode formed by a part of the EUT under test. There is a stray capacitance of about 1 pF to several pF depending on the surface area of the discharge electrode and the length of the discharge gap GAP.
At the beginning of spark discharge generation, the charge on the stray capacitance quickly disappears in the spark space, so the existence of the stray capacitance can be almost ignored. However, if the size of the stray capacitance is intentionally increased, the following operation occurs. It should be done.
即ち、放電間隙GAP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GAP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。 That is, at the beginning of the spark discharge in the discharge gap GAP, the charge of the charge/discharge capacitor C CD tries to be injected into the spark space via the discharge resistance R D , but due to the discharge resistance R D and the spark resistance in the discharge gap GAP, The amount of charge that is limited and injected into the spark space is extremely small.
然しながら、浮遊容量の電荷は放電抵抗RDに
関係なく放電間隙GAPにおける火花抵抗にのみ
制限されることとなるから、浮遊容量から火花空
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遥かに大となり、放
電間隙GAPにおける導電率の増大に伴つて浮遊
容量の電荷の全てが火花空間にのみ注入される。 However, since the charge of the stray capacitance is limited only by the spark resistance in the discharge gap GAP, regardless of the discharge resistance R D , the amount of charge injected from the stray capacitance into the spark space is equal to the charge/discharge capacitor C C D
The amount of charge injected from the spark gap is much larger than that of the spark, and as the conductivity in the discharge gap GAP increases, all of the charge in the stray capacitance is injected only into the spark space.
そして浮遊容量と放電間隙GAPとを結ぶ電流
径路のインピーダンスを小ならしめることによつ
て浮遊容量から火花空間への電荷の注入を速やか
ならしめることが出来、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GAP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に加え得ることとなる。 By reducing the impedance of the current path connecting the stray capacitance and the discharge gap GAP, charge can be quickly injected from the stray capacitance into the spark space, and most of the charge in the charge/discharge capacitor C CD is lost. By flashing the discharge gap GAP without causing any damage, almost all of the charge in the charging/discharging capacitor C CD can be applied to the EUT under test.
尚、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GAPを通して
放出される電流によつてのみ定まり、浮遊容量の
電荷には無関係である。 The energy applied to the EUT under test is
It is determined only by the current discharged from the charge/discharge capacitor C CD through the discharge gap GAP, and is independent of the charge of stray capacitance.
本考案は、放電間隙に存在する浮遊容量を意図
的に大ならしめるために放電間隙と並列に静電容
量素子を接続すると共に、この並列静電容量素子
と放電間隙とを結ぶ電流径路のインピーダンスを
極めて小ならしめることによつて、充放電コンデ
ンサの静電容量、放電抵抗の抵抗値、放電開始電
圧、即ち、放電間隙の長さ等を変化せしめた場合
においても放電電流の波形の歪及び放電電流の立
上り時間等の電気的特性を従来に比し著しく改善
し得ると共に、火花生成機構の不確定性によつて
放電毎に生ずる上記電気的特性のばらつきを極め
て小ならしめ得る静電気放電シミユレータを実現
することを目的とする。 This invention connects a capacitance element in parallel with the discharge gap in order to intentionally increase the stray capacitance existing in the discharge gap, and also reduces the impedance of the current path connecting this parallel capacitance element and the discharge gap. By making this extremely small, distortion of the waveform of the discharge current and An electrostatic discharge simulator that can significantly improve electrical characteristics such as the rise time of a discharge current compared to conventional ones, and that can extremely minimize variations in the electrical characteristics that occur for each discharge due to the uncertainty of a spark generation mechanism. The purpose is to realize the following.
第1図は、本考案の一実施例の要部を示す図
で、BED1,BED2及びBED3は鍔状対向電極、
CPは筒状接触体で、筒状導体の下端縁に鍔状導
体を一体に結合し、その外周縁を鍔状対向電極
BED1、BED2及びBED3の中の中央の電極BED2
の内周縁に固着してある。 FIG. 1 is a diagram showing the main parts of an embodiment of the present invention, in which BED 1 , BED 2 and BED 3 are flanged counter electrodes;
CP is a cylindrical contact body in which a flange-shaped conductor is integrally connected to the lower edge of the cylindrical conductor, and its outer periphery is connected to a flange-shaped counter electrode.
Central electrode BED 2 among BED 1 , BED 2 and BED 3
It is fixed to the inner periphery of the
尚、中央の電極BED2と筒状接触体CPとを別個
に形成した後、一体に結合する代りに、1枚の導
体板に絞り加工を施す等の手段よつて所要形状に
形成してもよい。 Incidentally, instead of forming the center electrode BED 2 and the cylindrical contact body CP separately and then joining them together, it is also possible to form them into the desired shape by drawing a single conductive plate or other means. good.
HEDは半球状電極で、適当な弾力性を有する
導体薄板を以て形成すると共に、その周辺部に放
射状の切込を設け、この周辺部を鍔状対向電極
BED3の内周辺に圧接せしめてある。 HED is a hemispherical electrode, which is formed from a conductive thin plate with appropriate elasticity, and has radial notches around its periphery, and this periphery is used as a brim-shaped counter electrode.
It is pressed against the inner periphery of BED 3 .
SUPは絶縁支持体で、適当な硬質合成樹脂等
より成り、鍔状対向電極BED1,BED2及びBED3
の各対向間隙内に充填すると共に、上部電極
BED1及び下部電極BED3の各外周に電極と一体
に設けてある。 SUP is an insulating support made of suitable hard synthetic resin, etc., and has flanged counter electrodes BED 1 , BED 2 and BED 3
The upper electrode
It is provided on each outer periphery of BED 1 and lower electrode BED 3 integrally with the electrode.
尚、沿面放電を防止するために、電極BED1の
内周縁と電極BED2の間及び電極BED3の内周縁
と電極BED2の間を絶縁支持体SUPの一部で覆つ
てある。FSは放電電極の支持及び放電間隙の調
整素子で、マイクロメータ等に用いられている送
り螺子機構より成り、回転操作つまみを正又は逆
方向に回転せしめることにより可動軸を前進又は
後退せしめ得ると共に、可動軸の移動距離を目盛
によつて指示し得るように形成してある。SUPT
は放電間隙の調整素子FSの支持用突出部で、絶
縁支持体SUPと同様の材質より成り、絶縁支持
体SUPの上面、即ち、鍔状対向電極BED1側の表
面に絶縁支持体SUPと一体に、かつ、鍔状対向
電極BED1,BED2及びBED3の板面とほぼ直角に
なるように突出せしめ、その内部に放電間隙の調
整素子FSを挿入し、支持具HWによつて固定し
てある。放電間隙の調整素子FSの可動軸は、支
持用突出部SUPTの内部において筒状接触体CP内
に挿入され、軸方向に滑動自在なると共に、筒状
接触体CPと電気的に接続される。 Note that, in order to prevent creeping discharge, a portion of the insulating support SUP covers the space between the inner peripheral edge of the electrode BED 1 and the electrode BED 2 , and between the inner peripheral edge of the electrode BED 3 and the electrode BED 2 . FS is an element that supports the discharge electrode and adjusts the discharge gap, and consists of a feed screw mechanism used in micrometers, etc., and can move the movable shaft forward or backward by rotating the rotation control knob in the forward or reverse direction. , so that the moving distance of the movable shaft can be indicated by a scale. SUP T
is a protrusion for supporting the discharge gap adjustment element FS, which is made of the same material as the insulating support SUP, and is integrated with the insulating support SUP on the upper surface of the insulating support SUP, that is, the surface on the brim-shaped counter electrode BED 1 side. The counter electrodes BED 1 , BED 2 and BED 3 are made to protrude almost perpendicularly to the plate surfaces of the counter electrodes BED 1 , BED 2 and BED 3 , and a discharge gap adjusting element FS is inserted therein and fixed with a support HW. There is. The movable shaft of the discharge gap adjustment element FS is inserted into the cylindrical contact body CP inside the support protrusion SUP T , is slidable in the axial direction, and is electrically connected to the cylindrical contact body CP. .
放電間隙の調整素子FSの可動軸を滑動自在な
らしめると共に、筒状接触体CPとの電気的接続
を確実ならしめるために、筒状接触体CPを弾力
性を有する導体を以て形成し、上端部に適当な軸
長に亙つて軸方向の切込みを設けて適宜数の圧着
片を形成せしめてもよい。SEDは放電電極で、
放電間隙の調整素子FSの可動軸の内端面に固定
して取り付け、半球状電極HEDと共に一対の放
電電極を構成する。NTは筒状のナツト部分で、
絶縁支持体SUPと同様の材質より成り、絶縁支
持体SUPの下面、即ち、鍔状対向電極BED3側の
面において半球状電極HEDの外側に絶縁支持体
SUPと一体にして突設せしめてある。ZSは零調
整螺子で、ナツト部分NTと同様の材質より成
り、ナツト部分NTに螺合せしめると共に、その
内端が半球状電極HEDに圧接するように形成し
てある。 In order to make the movable axis of the discharge gap adjustment element FS slidable and to ensure electrical connection with the cylindrical contact body CP, the cylindrical contact body CP is formed of an elastic conductor, and the upper end portion An appropriate number of crimp pieces may be formed by providing an axial notch over an appropriate axial length. SED is a discharge electrode,
It is fixedly attached to the inner end surface of the movable shaft of the discharge gap adjustment element FS, and forms a pair of discharge electrodes together with the hemispherical electrode HED. NT is a cylindrical nut part,
It is made of the same material as the insulating support SUP, and the insulating support is placed outside the hemispherical electrode HED on the lower surface of the insulating support SUP, that is, the surface on the side of the brim-shaped counter electrode BED 3 .
It is integrated with the SUP and installed protrudingly. ZS is a zero adjustment screw, made of the same material as the nut part NT, screwed onto the nut part NT, and formed so that its inner end is pressed into contact with the hemispherical electrode HED.
尚、零調整螺子ZSの中心軸と放電間隙の調整
素子FSの中心軸とをほぼ一致せしめることによ
つて、後述する零調整を正確に行うことが出来
る。CTTは棒状導体より成る接触子で、先端を
先鋭ならしめ、後端部を絶縁支持体SUPの外周
面から中心方向に設けた螺子孔に螺合せしめる
か、固く嵌入せしめ、後端部を中央の面が鍔状対
向電極BED2(接地側電極)の周縁、又は電極
BED2からの引出線等に電気的に接続されるよう
に取り付けてある。HOLは絶縁保持筒で、その
前端部に設けた孔隙部に絶縁支持体SUPの周辺
部を固く嵌入し、必要に応じて接着剤又は止め螺
子等を用いて絶縁保持筒HOLと絶縁支持体SUP
とを一体に結合せしめると共に、絶縁保持筒
HOLの中空内部に挿入された絶縁支持体SUPの
周辺部分の一部を切欠いて上部の鍔状対向電極
BED1及び下部の鍔状対向電極BED3の各周縁部
の一部を絶縁保持筒HOLの中空内部に露出せし
め、この部分において両電極を電気的に接続する
か、鍔状対向電極BED1及びBED3に各接続した
引出線の各端部を絶縁保持筒HOLの中空内部に
導入し、両引出線を電気的に接続してある。鍔状
対向電極BED1及びBED3は前記のような接続個
所の他、任意の周縁部分において互いに接続して
もよく、接触子CTTと中央の鍔状対向電極BED2
との接続部分を除く全周において電気的に接続し
てもよい。 Note that by making the center axis of the zero adjustment screw ZS substantially coincide with the center axis of the discharge gap adjustment element FS, the zero adjustment described later can be performed accurately. CTT is a contact made of a rod-shaped conductor.The tip is sharpened, the rear end is screwed into a screw hole provided from the outer circumferential surface of the insulating support SUP toward the center, or it is firmly inserted, and the rear end is centered The surface is the periphery of the brim-shaped counter electrode BED 2 (ground side electrode) or the electrode
It is installed so that it is electrically connected to the lead wire etc. from BED 2 . The HOL is an insulating holding cylinder, and the peripheral part of the insulating support SUP is firmly fitted into the hole provided at the front end of the HOL, and if necessary, the insulating holding cylinder HOL and the insulating support SUP are connected using adhesive or set screws.
and an insulating holding cylinder.
A part of the peripheral part of the insulating support SUP inserted into the hollow interior of the HOL is cut out to form a flanged counter electrode on the top.
A part of the peripheral edge of BED 1 and the lower brim-shaped counter electrode BED 3 is exposed in the hollow interior of the insulation holding cylinder HOL, and both electrodes are electrically connected at this part, or the brim-shaped counter electrode BED 1 and the lower brim-shaped counter electrode BED 3 are connected electrically. Each end of each lead wire connected to BED 3 is introduced into the hollow interior of the insulation holding cylinder HOL, and both lead wires are electrically connected. The brim-like counter electrodes BED 1 and BED 3 may be connected to each other at any peripheral portion in addition to the above connection points, and the contact CTT and the center brim-like counter electrode BED 2 may be connected to each other at any peripheral portion.
It may be electrically connected to the entire circumference except for the connection part.
尚、絶縁支持体SUPと絶縁保持筒HOLを一体
に結合せしめるに当つて、接触子CTTの軸方向
と絶縁保持筒HOLの軸方向とをほぼ一致せしめ
ることによつて放電試験時の取扱操作を容易なら
しめることが出来る。 In addition, when connecting the insulating support SUP and the insulating holding tube HOL together, the axial direction of the contactor CTT and the axial direction of the insulating holding tube HOL are made to almost match, thereby making handling operations during the discharge test easier. You can do it if it's easy.
図には示していないが、絶縁保持筒HOLの中
空内部に充放電コンデンサ及び放電抵抗を内装す
ると共に、絶縁保持筒HOLの後端部又は側壁等
から充電電源回路への接続線を導入し、充放電コ
ンデンサCCDの高電位側電極を放電抵抗を介して
鍔状対向電極BED1及びBED3(高圧側電極)に接
続すると共に、充電電源回路への接続線の中、高
電位側の接続線に接続し、又、充放電コンデンサ
CCDの低電位側電極を充電電源回路への接続線の
中、低電位側の接続線に接続し、更に、放電間隙
の調整素子FSの適宜個所又はその支持具HW或
は接触子CTTのように鍔状対向電極BED2(接地
側電極)と電気的に接続されている個所と、地気
間に適当な高抵抗を接続する。 Although not shown in the figure, a charging/discharging capacitor and a discharging resistor are installed inside the hollow interior of the insulating holding cylinder HOL, and a connecting wire to the charging power supply circuit is introduced from the rear end or side wall of the insulating holding cylinder HOL, Connect the high potential side electrode of the charge/discharge capacitor C CD to the flanged counter electrodes BED 1 and BED 3 (high voltage side electrode) via the discharge resistor, and connect the high potential side of the connection wire to the charging power supply circuit. Connect to the line and also charge/discharge capacitor
Connect the low-potential side electrode of C CD to the low-potential side connection wire among the connection wires to the charging power supply circuit, and then connect it to the appropriate part of the discharge gap adjusting element FS, its support HW, or the contactor CTT. Connect an appropriate high resistance between the point electrically connected to the brim-shaped counter electrode BED 2 (ground side electrode) and the ground air.
このように構成した本案静電気放電シミユレー
タにおいては、放電間隙の調整素子FSのつまみ
を操作して目盛を零に一致せしめ、零調整螺子
ZSを回転し、放電電極SEDを半球状電極HEDの
内底壁に密着させて零調整を行うが、放電電極
SEDと半球状電極HEDとの密着を検地するには、
例えば充電電源回路を開放状態に保ち、充電電源
回路への接続線の中、高電位側の接続線と、放電
間隙の調整素子FSの適宜個所又はその支持具
HW或は接触子CTT、即ち、放電電極SEDと電
気的に接続されている個所との間の遮断導通を回
路試験器等によつて検出する。即ち、零調整螺子
ZSを逆方向に回転してこれを後退せしめると、
半球状電極HEDの弾力により、その周辺部と鍔
状対向電極BED3との接触を保持した状態で頂部
が後退して放電電極SEDとの接触が断たれ、零
調整螺子ZSを正方向に回転し、半球状電極HED
の弾力に抗して零調整螺子ZSを前進せしめると、
半球状電極HEDの周辺部が鍔状対向電極BED3の
表面に圧接された状態で半径方向に摺動拡大しつ
つ変形し、その頂部が前進して放電電極SEDに
接触するに至るから回路試験器の指針の振れの変
化を読み取ることにより零調整の完了を確かめる
ことが出来る。 In the electrostatic discharge simulator of the present invention constructed in this way, the scale is made to match zero by operating the knob of the discharge gap adjustment element FS, and the zero adjustment screw is
Zero adjustment is performed by rotating ZS and bringing the discharge electrode SED into close contact with the inner bottom wall of the hemispherical electrode HED.
To detect the close contact between SED and hemispherical electrode HED,
For example, keep the charging power supply circuit in an open state, and connect the connection wire to the charging power supply circuit, the connection wire on the high potential side, and the appropriate parts of the discharge gap adjustment element FS or its support.
A circuit tester or the like is used to detect interruption or continuity between the HW or the contactor CTT, that is, the discharge electrode SED and the electrically connected location. That is, the zero adjustment screw
If you rotate ZS in the opposite direction and move it backwards,
Due to the elasticity of the hemispherical electrode HED, the top recedes while maintaining contact between its periphery and the flanged counter electrode BED 3 , breaking contact with the discharge electrode SED, and rotating the zero adjustment screw ZS in the positive direction. and hemispherical electrode HED
When the zero adjustment screw ZS is moved forward against the elasticity of
The peripheral part of the hemispherical electrode HED is pressed against the surface of the brim-shaped counter electrode BED 3 and deforms while sliding and expanding in the radial direction, and the top part moves forward and comes into contact with the discharge electrode SED, so the circuit test is performed. Completion of zero adjustment can be confirmed by reading changes in the deflection of the instrument's pointer.
零調整を終つた後、放電間隙の調整素子FSの
つまみを操作して放電間隙の長さを所要値に調整
し、接触子CTTの先端を被試験体の所要個所に
接触せしめて充放電コンデンサを充電すると、そ
の充電電圧が放電間隙の長さに対応する電圧に達
した際に放電が行われる。 After completing the zero adjustment, adjust the length of the discharge gap to the required value by operating the knob of the discharge gap adjustment element FS, and then touch the tip of the contactor CTT to the desired location on the test object to remove the charge/discharge capacitor. When charged, discharge occurs when the charging voltage reaches a voltage corresponding to the length of the discharge gap.
尚、第1図には、3枚の鍔状対向電極BED1,
BED2及びBED3によつて並列容量を形成した場
合を例示したが、電極BED1を省いて電極BED2
及びBED3によつて並列容量を形成しても本考案
を実施することが出来る。 In addition, in FIG. 1, three flanged counter electrodes BED 1 ,
Although the case where parallel capacitance is formed by BED 2 and BED 3 is illustrated, electrode BED 1 is omitted and electrode BED 2 is
The present invention can be implemented even if a parallel capacitance is formed by BED 3 and BED 3 .
(考案の効果)
本案静電気放電シミユレータにおいては、鍔状
対向電極BED1,BED2及びSED3によつて放電間
隙と並列の容量が形成されると共に、この並列容
量と放電間隙間は、一方の放電電極を形成する半
球状電極HED自体と、放電電極SED、放電間隙
の調整素子FSの可動軸及び筒状接触体CPとによ
つて接続されているので、この接続部分における
インピーダンスは極めて小である。(Effect of the invention) In the electrostatic discharge simulator of the present invention, a capacitance in parallel with the discharge gap is formed by the flanged counter electrodes BED 1 , BED 2 and SED 3 , and this parallel capacitance and the discharge gap are Since the hemispherical electrode HED that forms the discharge electrode is connected to the discharge electrode SED, the movable shaft of the discharge gap adjustment element FS, and the cylindrical contact body CP, the impedance at this connection part is extremely small. be.
そして充放電コンデンサの充電に際して、予め
接触子CTTを被試験体に接触せしめた状態で充
放電コンデンサを充電する場合には、絶縁保持筒
HOLに内装された放電抵抗、鍔状対向電極
BED1,BED3及びBED2、接触子CTT並に被試
験体を介して鍔状対向電極BED1,BED2及び
BED3より成る並列容量が充放電コンデンサと共
に充電され、接触子CTTを被試験体に接触せし
めない状態で充放電コンデンサを充電する場合に
は、放電間隙の調整素子FSの適宜個所又はその
支持具HW或は接触子CTT等のように鍔状対向
電極BED2と電気的に接続されている個所と地気
間に挿入した高抵抗及び絶縁保持筒HOLに内装
された放電抵抗を介して鍔状対向電極BED1,
BED2及びBED3より成る並列容量も亦充電され、
充放電コンデンサの放電時には、並列容量からの
電荷が大量に、かつ速やかに火花空間に注入さ
れ、充放電コンデンサの電荷を殆ど失うことなく
放電間隙を閃絡せしめて、充放電コンデンサの電
荷の殆ど全てを被試験体に加えることが出来、充
放電コンデンサの静電容量、放電抵抗の抵抗値及
び放電間隙の長さ等を変化せしめて実験を行つた
結果によれば、放電電流の立上り時間及び波形の
歪等の電気的特性を従来に比し著しく改善し、放
電毎における上記電気的特性のばらつきも極めて
小なることを確かめることが出来た。 When charging the charge/discharge capacitor, when charging the charge/discharge capacitor with the contactor CTT in contact with the test object in advance, the insulating holding tube
Discharge resistor and flanged counter electrode built into HOL
BED 1 , BED 3 and BED 2 , contactor CTT and flanged counter electrodes BED 1 , BED 2 and
When a parallel capacitor consisting of BED 3 is charged together with a charge/discharge capacitor and the charge/discharge capacitor is charged without contacting the contactor CTT with the test object, the discharge gap adjustment element FS or its support may be The high resistance inserted between the part electrically connected to the flanged counter electrode BED 2 such as HW or contactor CTT and the ground air, and the discharge resistor built into the insulation holding tube HOL, Counter electrode BED 1 ,
The parallel capacitance consisting of BED 2 and BED 3 is also charged,
When the charge/discharge capacitor is discharged, a large amount of charge from the parallel capacitor is quickly injected into the spark space, causing the discharge gap to flash without losing much of the charge/discharge capacitor's charge. According to the results of experiments conducted by changing the capacitance of the charge/discharge capacitor, the resistance value of the discharge resistor, the length of the discharge gap, etc., it was found that the rise time and It was confirmed that the electrical characteristics such as waveform distortion were significantly improved compared to the conventional method, and that the variation in the electrical characteristics between discharges was also extremely small.
尚、鍔状対向電極BED1,BED2及びBED3より
成る並列容量の充電のために設けた高抵抗の抵抗
値を被試験体のインピーダンスに比し適当に大な
らしめておけば、放電電流がこの高抵抗に分流す
るおそれはない。 Furthermore, if the resistance value of the high resistance provided for charging the parallel capacitance consisting of the brim-shaped counter electrodes BED 1 , BED 2 , and BED 3 is made appropriately larger than the impedance of the test object, the discharge current can be increased. There is no risk of the current being shunted to this high resistance.
第1図は、本考案の一実施例を示す図、第2図
は、従来の静電気放電シミユレータの一例を示す
図で、BED1,BED2及びBED3……鍔状対向電
極、CP……筒状接触体、HED……半球状電極、
SUP……絶縁支持体、FS……放電間隙の調整素
子、SUPT……突出部、HW……支持具、SED…
…放電電極、NT……ナツト部分、ZS……零調整
螺子、CTT……接触子、HOL……絶縁保持筒、
CCD……充放電コンデンサ、RD……放電抵抗、
GAP……放電間隙、EUT……被試験体である。
FIG . 1 is a diagram showing an embodiment of the present invention, and FIG . 2 is a diagram showing an example of a conventional electrostatic discharge simulator. Cylindrical contact body, HED... hemispherical electrode,
SUP...Insulating support, FS...Discharge gap adjustment element, SUP T ...Protrusion, HW...Support, SED...
...discharge electrode, NT...nut part, ZS...zero adjustment screw, CTT...contact, HOL...insulation holding cylinder,
C CD ...Charging/discharging capacitor, R D ...Discharging resistor,
GAP...discharge gap, EUT...test object.
Claims (1)
と、この鍔状対向電極の中、接地側電極の中央部
分に一体に設けた筒状接触体と、前記鍔状対向電
極の外周に設けた絶縁支持体と、この絶縁支持体
に支持され、可動軸を前記筒状接触体と接触を保
つて滑動自在ならしめた送り螺子機構より成る放
電間隙の調整素子と、この放電間隙の調整素子に
おける可動軸の内端に取り付けた放電電極と、前
記鍔状対向電極の中、高圧側電極の内周辺に、周
辺部を圧接され、前記放電電極と対向せしめられ
る半球状電極と、前記絶縁支持体の一部に突設し
た筒状部分に螺合され、その内端を前記半球状電
極に圧接せしめられる零調整螺子と、前記絶縁支
持体の周縁部に挿通支持され、後端部を前記鍔状
対向電極の中の接地側電極に接続される導体より
成る接触子と、放電抵抗を介して前記鍔状対向電
極の中の高圧側電極に接続される充放電コンデン
サを内装し、前記絶縁支持体に取り付けられた絶
縁保持筒とを備えたことを特徴とする静電気放電
シミユレータ。 A flange-shaped counter electrode facing each other at an appropriate interval, a cylindrical contact body integrally provided in the center portion of the ground side electrode within the flange-shaped counter electrode, and an insulator provided on the outer periphery of the flange-shaped counter electrode. a support, a discharge gap adjusting element supported by the insulating support and having a movable shaft slidably slidable while maintaining contact with the cylindrical contact body; and a discharge gap adjusting element that is movable in the discharge gap adjusting element. A discharge electrode attached to the inner end of the shaft, a hemispherical electrode whose peripheral portion is pressure-welded to the inner periphery of the high-voltage side electrode in the brim-shaped counter electrode and is opposed to the discharge electrode, and the insulating support. A zero adjustment screw is screwed into a partially protruding cylindrical portion and has its inner end pressed into contact with the hemispherical electrode; A contact made of a conductor connected to the ground side electrode in the counter electrode, and a charging/discharging capacitor connected to the high voltage side electrode in the flanged counter electrode via a discharge resistor are installed inside the insulating support. An electrostatic discharge simulator characterized by comprising: an insulating holding tube attached to the simulator.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17041785U JPH0435817Y2 (en) | 1985-11-07 | 1985-11-07 |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17041785U JPH0435817Y2 (en) | 1985-11-07 | 1985-11-07 |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6279176U JPS6279176U (en) | 1987-05-20 |
| JPH0435817Y2 true JPH0435817Y2 (en) | 1992-08-25 |
Family
ID=31105128
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP17041785U Expired JPH0435817Y2 (en) | 1985-11-07 | 1985-11-07 |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0435817Y2 (en) |
-
1985
- 1985-11-07 JP JP17041785U patent/JPH0435817Y2/ja not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6279176U (en) | 1987-05-20 |
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