JPH0528532Y2 - - Google Patents
Info
- Publication number
- JPH0528532Y2 JPH0528532Y2 JP893986U JP893986U JPH0528532Y2 JP H0528532 Y2 JPH0528532 Y2 JP H0528532Y2 JP 893986 U JP893986 U JP 893986U JP 893986 U JP893986 U JP 893986U JP H0528532 Y2 JPH0528532 Y2 JP H0528532Y2
- Authority
- JP
- Japan
- Prior art keywords
- discharge
- conductor
- shaped
- charging
- 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 - Lifetime
Links
- 239000004020 conductor Substances 0.000 claims description 48
- 239000003990 capacitor Substances 0.000 claims description 38
- 238000007599 discharging Methods 0.000 description 28
- 239000008186 active pharmaceutical agent Substances 0.000 description 6
- 238000010586 diagram Methods 0.000 description 4
- 229920003002 synthetic resin Polymers 0.000 description 4
- 239000000057 synthetic resin Substances 0.000 description 4
- 230000007423 decrease Effects 0.000 description 3
- 230000015572 biosynthetic process Effects 0.000 description 2
- 230000037237 body shape Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000005684 electric field Effects 0.000 description 2
- 239000007769 metal material Substances 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 230000015556 catabolic process Effects 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 239000013013 elastic material Substances 0.000 description 1
- 230000005611 electricity Effects 0.000 description 1
- 230000005674 electromagnetic induction Effects 0.000 description 1
- 230000006698 induction Effects 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 230000000630 rising effect Effects 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 230000003068 static effect Effects 0.000 description 1
Landscapes
- Testing Electric Properties And Detecting Electric Faults (AREA)
- Tests Of Electronic Circuits (AREA)
- Testing Of Individual Semiconductor Devices (AREA)
- Testing Relating To Insulation (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) Electrostatic discharges to the various electronic circuits, components, and various electronic devices described above are most often caused by static electricity being discharged from a charged body made of a conductor insulated from the ground, particularly the human body, and therefore most electrostatic discharge simulators use an equivalent model 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 discharge 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
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. During the spark discharge generation process, the electric field strength in the spark space decreases, and this decrease in electric field strength weakens the effect of increasing conductivity, causing the conductivity to increase along the trajectory corresponding to the original rise time. is no longer performed, and the rise time of the discharge current becomes shorter than the discharge gap.
There is a significant delay compared to the fixed time determined depending on the length of the GAP and the atmospheric pressure, and 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
経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経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 discharge current compared to conventional ones, and can also minimize variations in the electrical characteristics that occur from discharge to discharge due to uncertainty in the 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、BOWは椀状支持導体、BEDは鍔状電極で、
椀状支持導体BOWの周縁部に一体に取り付けて
ある。GUDは軸方向のキー溝KGを有する案内筒
で、椀状支持導体BOWの頂部に一体に取り付け
ると共に、椀状支持導体BOWのほぼ中心部に穿
つた孔隙のキー溝と案内筒GUDのキー溝KGとの
位置が一致するように結合せしめてある。INSs
は絶縁層で、椀状支持導体BOWの内外表面、鍔
状電極BEDの表裏面、その周縁部及び案内筒
GUDの外周面に亙つて一体に設け、椀状支持導
体BOWのほぼ中心部に穿つたキー溝付き孔隙に
対応する個所には、この孔隙と同一の大きさでキ
ー溝の位置の一致するキー溝付き孔隙を設けてあ
る。 FIG. 1 is a diagram showing the main parts of an embodiment of the present invention, in which BOW is a bowl-shaped supporting conductor, BED is a brim-shaped electrode,
It is integrally attached to the periphery of the bowl-shaped support conductor BOW. GUD is a guide tube with an axial keyway KG, which is integrally attached to the top of the bowl-shaped support conductor BOW, and the keyway of the hole bored in the approximate center of the bowl-shaped support conductor BOW and the keyway of the guide tube GUD. It is connected so that the position matches with KG. INS s
is an insulating layer, which covers the inner and outer surfaces of the bowl-shaped supporting conductor BOW, the front and back surfaces of the brim-shaped electrode BED, its periphery, and the guide tube.
A key groove with the same size and key groove position as the hole is provided integrally over the outer circumferential surface of the GUD at a location corresponding to a hole with a key groove bored approximately in the center of the bowl-shaped support conductor BOW. A grooved hole is provided.
尚、椀状支持導体BOW及び案内筒GUDを比較
的肉厚の導体を以て剛体状に形成し、鍔状電極
BEDを比較的柔軟性を有する導体を以て形成す
ると共に、絶縁層INSsをゴム弾性体を以て形成
するか、椀状支持導体BOW、案内筒GUD及び鍔
状電極BEDを全て柔軟性を有する導体を以て形
成すると共に、絶縁層INSsの中、椀状支持導体
BOW及び案内筒GUDの表面に対応する絶縁層部
分を硬質の絶縁合成樹脂等を以て形成し、鍔状電
極BEDの表面に対応する絶縁層部分を軟質の絶
縁合成樹脂を以て形成することにより、椀状支持
導体BOW及び案内筒GUD部分を剛体状に形成
し、鍔状電極BED部分を柔軟性を有するように
形成することが最も望ましいが、全体を剛体状に
形成しても本考案を実施することが出来る。 In addition, the bowl-shaped support conductor BOW and the guide tube GUD are formed into a rigid body using a relatively thick conductor, and the flange-shaped electrode
The BED is formed of a relatively flexible conductor, and the insulating layer INS is formed of a rubber elastic material, or the bowl-shaped supporting conductor BOW, the guide tube GUD, and the brim-shaped electrode BED are all formed of a flexible conductor. At the same time, a bowl-shaped supporting conductor is placed inside the insulating layer INS s.
By forming the insulating layer portions corresponding to the surfaces of the BOW and guide cylinder GUD using a hard insulating synthetic resin, etc., and forming the insulating layer portion corresponding to the surface of the brim-shaped electrode BED using a soft insulating synthetic resin, a bowl-shaped Although it is most desirable to form the support conductor BOW and the guide tube GUD part in a rigid body shape, and to form the brim electrode BED part in a flexible manner, the present invention can also be implemented even if the entire body is formed in a rigid body shape. I can do it.
又、上記のように案内筒GUDを導体を以て形
成する代りに、絶縁硬質合成樹脂を以て形成して
もよい。 Further, instead of forming the guide tube GUD from a conductor as described above, it may be formed from an insulating hard synthetic resin.
SUPは棒状可動導体で、その前半部に軸方向
の突起KYを設け、後半部に螺子を刻み、軸方向
の突起KYを案内筒GUDのキー溝KGに一致せし
めて案内筒GUDに挿通することにより、椀状支
持導体BOWとの電気的接続を保持して軸方向に
滑動し得るように形成してある。SEDは放電電
極で、棒状可動導体SUPの前端に取り付けてあ
る。HOLは筒状絶縁支持体、HANは把手で、筒
状絶縁支持体HOLに一体に取り付けてある。DS
は送り螺子で、螺子本体と、その背部に設けた鍔
状突起との間に、筒状絶縁支持体HOLの前端壁
に穿つた孔隙の内周辺を介在せしめることによ
り、送り螺子DSを筒状絶縁支持体HOLの前端壁
に回転自在に支持すると共に、棒状可動導体
SUPの後半部に設けた螺子に螺合せしめてある。
送り螺子DSは硬質の絶縁合成樹脂又は適当な金
属材料を以て形成し、金属材料を以て形成する場
合には、外表面に絶縁層を設けること椀状支持導
体BOW等と同様である。EUTは被試験体、
INSEはその表面に設けられた絶縁層である。 SUP is a rod-shaped movable conductor, with an axial protrusion KY provided on the front half and a screw cut on the rear half, so that the axial protrusion KY matches the keyway KG of the guide tube GUD and is inserted into the guide tube GUD. It is formed so that it can slide in the axial direction while maintaining electrical connection with the bowl-shaped support conductor BOW. The SED is a discharge electrode attached to the front end of the rod-shaped movable conductor SUP. HOL is a cylindrical insulating support, and HAN is a handle, which is integrally attached to the cylindrical insulating support HOL. DS
is a feed screw, and by interposing the inner periphery of a hole drilled in the front end wall of the cylindrical insulating support HOL between the screw body and the flange-like protrusion provided on its back, the feed screw DS can be shaped into a cylindrical shape. It is rotatably supported on the front end wall of the insulating support HOL, and the rod-shaped movable conductor
It is screwed onto the screw provided on the rear half of the SUP.
The feed screw DS is formed of a hard insulating synthetic resin or a suitable metal material, and when formed of a metal material, an insulating layer is provided on the outer surface in the same manner as the bowl-shaped supporting conductor BOW. The EUT is the object under test,
INS E is an insulating layer provided on its surface.
図には示していないが、筒状絶縁支持体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、絶縁把手HANを介して充電電源
回路への接続線及び帰線を導入し、接続線の中、
高電位側の線をバツフア抵抗を介して充放電コン
デンサの高電位側電極に接続し、接続線の中、低
電位側の線を充放電コンデンサの低電位側電極に
接続すると共に、充放電コンデンサの高電位側電
極を放電抵抗を介して棒状可動導体SUPの後端
部に接続し、充放電コンデンサの低電位側電極に
帰線の内端を接続してある。 Although not shown in the figure, the cylindrical insulating support HOL
A charging/discharging capacitor and a discharging resistor are installed inside the hollow, and a connecting wire and a return wire to the charging power supply circuit are introduced through the insulating handle HAN, and inside the connecting wire,
Connect the high potential side wire to the high potential side electrode of the charge/discharge capacitor via a buffer resistor, and connect the low potential side wire of the connection wire to the low potential side electrode of the charge/discharge capacitor. The high potential side electrode of is connected to the rear end of the rod-shaped movable conductor SUP via a discharge resistor, and the inner end of the return wire is connected to the low potential side electrode of the charging/discharging capacitor.
本案静電気放電シミユレータにおいても充放電
コンデンサの等価静電容量を50pF乃至250pF、放
電抵抗の等価抵抗を100Ω乃至1500Ωの各範囲か
ら適当な固定値を選択し、又、図には示していな
いが、充電電源回路を高圧直流源、電源スイツチ
及び充電抵抗等を以て形成し、充放電コンデンサ
の充電電圧を0V乃至30数kVの範囲に亙つて適宜
設定し得るように構成してある。 In the electrostatic discharge simulator of this invention, the equivalent capacitance of the charge/discharge capacitor is selected from a range of 50 pF to 250 pF, and the equivalent resistance of the discharge resistor is selected from a range of 100 Ω to 1500 Ω. The charging power supply circuit is formed of a high-voltage DC source, a power switch, a charging resistor, etc., and is configured so that the charging voltage of the charging/discharging capacitor can be set appropriately over a range of 0V to 30-odd kV.
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、送り螺子DSを逆方向に回転せし
めて棒状可動導体SUP及び放電電極SEDを最大
限に後退せしめ、被試験体EUTの接地端子又は
筐体壁等の中、接地可能な個所を接地すると共
に、帰線の外端を被試験体EUTの接地端子又は
接地可能な個所に接続し、所要の放電点に放電電
極SEDを正対せしめて鍔状電極BED部分を被試
験体EUTの表面に密着せしめ、充放電コンデン
サを所要電圧に充電した後、充電電源回路を開放
し、送り螺子DSを正方向に回転せしめて棒状可
動導体SUP及び放電電極SEDを徐々に前進せし
めると、放電電極SEDと、この放電電極SEDが
正対する被試験体EUT部分の一部導体によつて
形成される放電電極との間における放電間隙の長
さが、空気及び被試験体EUTの表面における絶
縁層INSEの材質によつて定まる絶縁破壊間隙長
に達した際に生ずる火花放電によつて充放電コン
デンサの電荷が瞬間的に被試験体EUTに加えら
れ、帰線を介して充放電コンデンサに戻る。 In the electrostatic discharge simulator of the present invention configured in this way, the feed screw DS is rotated in the opposite direction to retract the rod-shaped movable conductor SUP and the discharge electrode SED to the maximum extent, and the ground terminal of the EUT under test or the wall of the housing, etc. In addition to grounding the middle and grounding points, connect the outer end of the return wire to the grounding terminal of the EUT under test or to the grounding point, and connect the discharge electrode SED directly to the required discharge point to connect the flanged electrode BED. After the part is brought into close contact with the surface of the EUT under test and the charging/discharging capacitor is charged to the required voltage, the charging power supply circuit is opened and the feed screw DS is rotated in the positive direction to gradually disconnect the bar-shaped movable conductor SUP and the discharge electrode SED. When the discharge electrode SED is moved forward to The spark discharge that occurs when the dielectric breakdown gap length determined by the material of the insulating layer INS E on the surface of the EUT is reached causes the electric charge of the charging/discharging capacitor to be instantaneously applied to the EUT under test, and is transferred via the return wire. and return to the charge/discharge capacitor.
尚、この放電時に、充放電コンデンサの高電位
側電極の電位低下に応じて充電電源回路への接続
線から放射されようとする電磁エネルギは、バツ
フア抵抗によつてその放射を抑えられ、放電試験
に誤差を与えるおそれはない。 During this discharge, the electromagnetic energy that is about to be radiated from the connection line to the charging power supply circuit as the potential of the high-potential side electrode of the charging/discharging capacitor decreases is suppressed by the buffer resistor, and the discharge test There is no risk of giving an error.
前記のように、放電間隙長を大ならしめた状態
で充放電コンデンサの充電を行つた後、放電間隙
を徐々に狭めて放電を生ぜしめる代りに、鍔状電
極BED部分を被試験体EUTの表面に密着せしめ
ると共に放電間隙を予め適宜の長さに調整した
後、充放電コンデンサの充電を行うようにすれ
ば、充放電コンデンサの充電電圧が放電間隙にお
ける放電開始電圧に達した際に火花放電を生ずる
が、この場合には、放電後、直に充放電コンデン
サの再充電が行われ、充電電源回路を開放するま
で放電が繰り返し行われることとなる。 As mentioned above, after charging the charge/discharge capacitor with the discharge gap length increased, instead of gradually narrowing the discharge gap to cause discharge, the flange-shaped electrode BED portion is connected to the EUT under test. If the charging/discharging capacitor is charged after the charging/discharging capacitor is brought into close contact with the surface and the discharge gap is adjusted to an appropriate length in advance, a spark discharge will occur when the charging voltage of the charging/discharging capacitor reaches the discharge starting voltage at the discharge gap. However, in this case, the charging/discharging capacitor is immediately recharged after discharging, and discharging is repeated until the charging power supply circuit is opened.
この場合にも、例えば放電回路に電磁誘導素子
又は静電誘導素子を設けて放電電流を検出し、こ
の検出出力によつて充電電源回路を自動的に開放
するように構成することによつて放電を1回に限
定することが出来る。 In this case, for example, an electromagnetic induction element or an electrostatic induction element is provided in the discharge circuit to detect the discharge current, and the charging power supply circuit is automatically opened based on this detection output. can be limited to one time.
(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SED及びこの放電電極SEDと正対する被試
験体EUTの一部導体部分により形成される放電
電極との間に放電間隙が形成され、鍔状電極
BED及びこの鍔状電極BEDと対向する被試験体
EUTの一部導体部分の間に静電容量が形成され、
更に、この静電容量は鍔状電極BED、椀状支持
導体BOW、棒状可動導体SUPを介して放電電極
SEDに接続されると共に、被試験体EUT側にお
いても静電容量形成に関与する導体部分と、放電
電極形成に関与する導体部分とが、その間に介在
する導体部分によつて接続されるので、鍔状電極
BED及びこれに対応する被試験体EUT側の一部
導体により形成される静電容量は、放電電極
SED及びこれに対応する被試験体EUT側の一部
導体により形成される放電間隙に並列に接続され
ることとなり、その接続回路のインピーダンスは
極めて小である。(Effect of the invention) In the electrostatic discharge simulator of the present invention, a discharge gap is formed between the discharge electrode SED and the discharge electrode formed by a part of the conductor part of the EUT under test that directly faces the discharge electrode SED, and the discharge gap is formed in the shape of a flange. electrode
BED and the test object facing this brim-shaped electrode BED
Capacitance is formed between some conductor parts of the EUT,
Furthermore, this capacitance is transferred to the discharge electrode via the brim-shaped electrode BED, the bowl-shaped support conductor BOW, and the rod-shaped movable conductor SUP.
In addition to being connected to the SED, the conductor part that is involved in capacitance formation and the conductor part that is involved in discharge electrode formation on the EUT side under test are connected by the conductor part that is interposed between them. Flange-shaped electrode
The capacitance formed by the BED and the corresponding part of the conductor on the EUT side is the discharge electrode.
It is connected in parallel to the discharge gap formed by the SED and a corresponding part of the conductor on the side of the EUT under test, and the impedance of the connected circuit is extremely small.
そして充放電コンデンサの充電に際して、放電
抵抗、棒状可動導体SUP、椀状支持導体BOW、
鍔状電極BED、被試験体EUTの一部導体及び地
気を介して鍔状電極BEDとこれに対向する被試
験体EUTの一部導体により形成される並列容量
も亦充放電コンデンサと同電圧に充電され、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
隙を閃路せしめて、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, a discharge resistor, a rod-shaped movable conductor SUP, a bowl-shaped support conductor BOW,
The parallel capacitance formed by the flange-shaped electrode BED, a part of the conductor of the EUT under test, and the part of the conductor of the EUT under test that faces the flange-shaped electrode BED through the ground air also has the same voltage as the charging/discharging capacitor. 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 discharge current It was confirmed that the electrical characteristics such as rise time and waveform distortion were significantly improved compared to the conventional ones, and the variation in the electrical characteristics between discharges was also extremely small.
尚、棒状可動導体SUPを送り螺子機構によつ
て前進後退せしめるように構成する代りに、棒状
可動導体SUPの後端部を筒状絶縁支持体HOLの
前端部に固定して取り付けると共に、案内筒
GUD及び椀状支持導体BOWに挿通し、絶縁把手
HAN又は筒状絶縁支持体HOLを前後に移動せし
めることにより棒状可動導体SUPを前進後退せ
しめるように構成してもよく、又、このように構
成する場合には案内筒GUDを省いてもよい。 In addition, instead of configuring the rod-shaped movable conductor SUP to be moved forward and backward by a feed screw mechanism, the rear end of the rod-shaped movable conductor SUP is fixedly attached to the front end of the cylindrical insulating support HOL, and the guide cylinder is
Insert into GUD and bowl-shaped support conductor BOW, insulated handle
The rod-shaped movable conductor SUP may be moved forward and backward by moving the HAN or the cylindrical insulating support HOL back and forth, and in this case, the guide tube GUD may be omitted.
以上は、被試験体EUTの表面が絶縁層INSEで
覆われている場合について説明したが、鍔状電極
BED部分を絶縁層INSsで覆つてあるので、被試
験体EUTの表面が絶縁層で覆われることなく、
導体が直接露出している場合においても前記と同
様にして放電試験を行うことが出来る。 Above, we have explained the case where the surface of the EUT under test is covered with the insulating layer INS E , but the flange-like electrode
Since the BED part is covered with an insulating layer , the surface of the EUT under test is not covered with an insulating layer.
Even when the conductor is directly exposed, a discharge test can be performed in the same manner as above.
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、BOW……椀状支持導体、BED……鍔状電
極、GUD……案内筒、KG……キー溝、INSs…
…絶縁層、SUP……棒状可動導体、KY……突
起、SED……放電電極、HOL……筒状絶縁支持
体、HAN……絶縁把手、DS……送り螺子、
EUT……被試験体、INSE……絶縁層、CCD……
充放電コンデンサ、RD……放電抵抗、GAP……
放電間隙である。
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, in which BOW...bowl-shaped support conductor, BED...flange-shaped electrode, GUD... Guide tube, KG...Keyway, INS s ...
...insulating layer, SUP...rod-shaped movable conductor, KY...protrusion, SED...discharge electrode, HOL...cylindrical insulating support, HAN...insulating handle, DS...feeding screw,
EUT...Test object, INS E ...Insulating layer, C CD ...
Charge/discharge capacitor, R D ……Discharge resistance, GAP……
This is the discharge gap.
Claims (1)
層で覆われた鍔状電極と、前記椀状支持導体に滑
動自在に支持された棒状可動導体と、この棒状可
動導体の前端部に取り付けられた放電電極と、前
記棒状可動導体の後部を支持し、中空内部に放電
抵抗及び充放電コンデンサを内装する筒状絶縁支
持体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 electrode provided integrally around the periphery of the bowl-shaped support conductor and covered with an insulating layer, a rod-shaped movable conductor slidably supported by the bowl-shaped support conductor, and attached to the front end of the rod-shaped movable conductor. 1. An electrostatic discharge simulator comprising: a discharge electrode having a cylindrical shape; and a cylindrical insulating support body that supports the rear part of the rod-shaped movable conductor and houses a discharge resistor and a charge/discharge capacitor in its hollow interior.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP893986U JPH0528532Y2 (en) | 1986-01-27 | 1986-01-27 |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP893986U JPH0528532Y2 (en) | 1986-01-27 | 1986-01-27 |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62121582U JPS62121582U (en) | 1987-08-01 |
| JPH0528532Y2 true JPH0528532Y2 (en) | 1993-07-22 |
Family
ID=30793786
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP893986U Expired - Lifetime JPH0528532Y2 (en) | 1986-01-27 | 1986-01-27 |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0528532Y2 (en) |
-
1986
- 1986-01-27 JP JP893986U patent/JPH0528532Y2/ja not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62121582U (en) | 1987-08-01 |
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