JP2557704B2 - Electrostatic characteristic evaluation device - Google Patents

Electrostatic characteristic evaluation device

Info

Publication number
JP2557704B2
JP2557704B2 JP1049483A JP4948389A JP2557704B2 JP 2557704 B2 JP2557704 B2 JP 2557704B2 JP 1049483 A JP1049483 A JP 1049483A JP 4948389 A JP4948389 A JP 4948389A JP 2557704 B2 JP2557704 B2 JP 2557704B2
Authority
JP
Japan
Prior art keywords
measured
discharge
static electricity
potential
potential difference
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 - Fee Related
Application number
JP1049483A
Other languages
Japanese (ja)
Other versions
JPH0328776A (en
Inventor
隆幸 加藤
英男 荒川
皓 久野
芳朗 梅本
秀樹 大野
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Toyota Motor Corp
Toyota Central R&D Labs Inc
Original Assignee
Toyota Motor Corp
Toyota Central R&D Labs Inc
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Toyota Motor Corp, Toyota Central R&D Labs Inc filed Critical Toyota Motor Corp
Priority to JP1049483A priority Critical patent/JP2557704B2/en
Publication of JPH0328776A publication Critical patent/JPH0328776A/en
Application granted granted Critical
Publication of JP2557704B2 publication Critical patent/JP2557704B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は物体に帯電する静電気を除電し、抑制するた
めの帯電防止手段の開発に役立つ帯電体の静電気特性を
正確に把握する評価装置に係り、特に、自動車シートに
用いられるファブリック材の静電気特性を精度良く簡便
に計測する静電気特性評価装置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Industrial field of application] The present invention relates to an evaluation device for accurately grasping the electrostatic characteristics of a charged body, which is useful for developing an antistatic means for eliminating and suppressing static electricity charged on an object. In particular, the present invention relates to an electrostatic characteristic evaluation device that accurately and simply measures electrostatic characteristics of fabric materials used for automobile seats.

〔従来技術〕[Prior art]

物体への静電気発生を防止することを目的とした帯電
防止手段として従来、物体に導電性を与えて、アース側
へ帯電した静電気を逃がす手段が一般的に用いられてい
る。例えば、自動車におけるシートファブリックでは、
導電性繊維を混入したり、或いは親水性の界面活性剤等
を付与して、導電性を持たせることが知られている。し
かし、導電性繊維の構造やその混入率或いは使用環境等
によつて、帯電防止効果すなわち、除電性能が大きく変
わる。そこで、各種帯電防止手段の開発においては、物
体に帯電した静電気の除電性能の評価が重要となる。
As an antistatic means for preventing the generation of static electricity on an object, conventionally, a means of giving conductivity to the object to release static electricity charged to the ground side has been generally used. For example, in seat fabrics for cars,
It is known that conductive fibers are mixed or a hydrophilic surfactant or the like is added to impart conductivity. However, the antistatic effect, that is, the static elimination performance greatly changes depending on the structure of the conductive fiber, the mixing ratio thereof, the usage environment, and the like. Therefore, in developing various antistatic means, it is important to evaluate the static elimination performance of static electricity charged on an object.

従来、この帯電防止手段における除電性能を評価する
ものとしては被測定物を5000Vに帯電させた後、被測定
物をアースして、被測定物の表面電位が50V以下になる
までの時間を計測し、その静電気減衰時間が2秒以下で
あれば被測定物の除電性能は良く、帯電しにくいと判断
する静電気減衰試験手段がある。さらに、被測定物体面
上を所望ピッチで走査する2個の表面電位検出手段を備
え、該表面電位検出手段の走査ピッチを表面電位の変化
の有無に応じて可変とし、第1の表面電位検出手段によ
って被測定物表面上に電位変化が検出されると、当該部
分のみを第2の表面電位検出手段を細いピッチで走査し
て、その電位分布を測定するようにした表面電位検出手
段がある(特開昭62−90565号)。
Conventionally, in order to evaluate the static elimination performance in this antistatic means, after charging the measured object to 5000 V, ground the measured object and measure the time until the surface potential of the measured object becomes 50 V or less. However, if the static electricity decay time is 2 seconds or less, there is a static electricity decay test means for judging that the charge removal performance of the measured object is good and it is difficult to be charged. Furthermore, two surface potential detecting means for scanning the surface of the object to be measured at a desired pitch are provided, and the scanning pitch of the surface potential detecting means is made variable according to the presence or absence of a change in the surface potential to detect the first surface potential. When a potential change is detected on the surface of the object to be measured by the means, there is a surface potential detecting means for measuring the potential distribution by scanning the second surface potential detecting means only at the portion at a fine pitch. (JP-A-62-90565).

〔従来技術の問題点〕[Problems of conventional technology]

前記静電気減衰試験手段は、被測定物体を測定用ホル
ダーに納めて帯電させた後、測定ホルダーをアースし
て、静電気を放電させた時の規定電圧までに低下するに
要する放電時間を計測するものであり、この手段では被
測定物全体からの静電気放電時間が測定される。従っ
て、被測定物の構造等による部分的な放電時間の違い
や、帯電した静電気の放電路の方向性等を評価すること
はできないという実用上の問題があった。
The static electricity decay test means measures the discharge time required to drop to a specified voltage when static electricity is discharged after the object to be measured is placed in a measurement holder and charged, and then the measurement holder is grounded. With this means, the electrostatic discharge time from the entire measured object is measured. Therefore, there is a practical problem that it is not possible to evaluate the partial difference in discharge time due to the structure of the object to be measured and the directionality of the discharge path of the charged static electricity.

また、表面電位分布測定装置は、第1の表面電位計測
手段を大きいピッチで走査させて、表面電位変化を検出
しているが、このためには、1個の表面電位検出手段で
時間間隔をおいて2回電位の計測を行い、前回データと
今回データの比較から電位変化を求める必要がある。従
って、データ蓄積機構が必要となり、装置が複雑にな
る。更に、データ比較の都合上実時間の電位差測定は不
可能となり、静電気放電時のような急峻な電圧降下の電
位差測定はできないという実用上の不都合を有する。
Further, the surface potential distribution measuring device scans the first surface potential measuring means at a large pitch to detect the surface potential change. For this purpose, one surface potential detecting means sets a time interval. It is necessary to measure the potential twice in advance and obtain the potential change by comparing the previous data and the current data. Therefore, a data storage mechanism is required, and the device becomes complicated. Furthermore, there is a practical inconvenience that the potential difference measurement in real time becomes impossible for the convenience of data comparison and the potential difference measurement of a steep voltage drop such as during electrostatic discharge cannot be performed.

〔発明が解決しようとする課題〕[Problems to be Solved by the Invention]

本発明は上記従来技術の問題点を解消するもので、被
測定物上の一点に放電用の電極を接続して、被測定物に
帯電した静電気をアースに放電させる手段と成すことに
より、当該放電電極の位置を変更して帯電防止手段によ
る静電気の放電速度の差や放電経路を検知することがで
きる。すなわち導電性繊維を混入する帯電防止ファブリ
ックでは該導電性繊維の混入法や織り方などによって局
部的に静電気の放電速度や放電経路が異なる。
The present invention solves the above-mentioned problems of the prior art, by connecting an electrode for discharge to one point on the DUT, and by forming a means for discharging the static electricity charged on the DUT to the ground, By changing the position of the discharge electrode, it is possible to detect the difference in the discharge rate of static electricity by the antistatic means and the discharge path. That is, in an antistatic fabric in which conductive fibers are mixed, the discharge rate and discharge path of static electricity are locally different depending on the method of mixing the conductive fibers and the weave.

従って、本発明によれば被測定物上の任意位置から、
その静電気を放電させることができ、被測定物の除電性
能を評価かつ正確に効率良く評価できる装置を提供する
ことを目的とする。
Therefore, according to the present invention, from an arbitrary position on the DUT,
It is an object of the present invention to provide an apparatus capable of discharging the static electricity and evaluating the charge removal performance of the object to be measured and accurately and efficiently.

さらに、本発明は、複数の表面電位計の差出力から被
測定物上の所定距離隔てた相互間の静電気の電位差を測
定することにより、電位差を実時間で計測できると共
に、放電時のような急峻な電圧降下時に発生する極めて
短時間の電位差をも正確に計測でき、かつ当該相互間の
電位差の発生期間から被測定物上の複数点間における静
電気の移動状態すなわち電荷の移動速度を検出可能とな
し帯電防止手段としての最適な導電率の与え方など、除
電性能の基礎的なデータを測定できるという実用上極め
て効果的な評価装置を提供することを目的とする。
Further, according to the present invention, the potential difference can be measured in real time by measuring the potential difference of static electricity between a plurality of surface electrometers which are separated by a predetermined distance from the difference output of the surface electrometer, and at the time of discharging. It is possible to accurately measure even a very short time potential difference that occurs when there is a sharp voltage drop, and it is possible to detect the static electricity movement state between multiple points on the DUT, that is, the charge movement speed, from the period of occurrence of the potential difference between them. It is an object of the present invention to provide a practically extremely effective evaluation device capable of measuring basic data of static elimination performance, such as how to give an optimum conductivity as an antistatic means.

〔発明の構成〕[Structure of Invention]

本発明の帯電体の静電気特性評価装置は、被測定物に
帯電した静電気を強制的に放電させた時の放電状態を複
数の表面電位計で計測し、その静電気の放電速度(時定
数)の大きさと、前記複数の表面電位計の出力差から求
める電位差の大きさとから被測定物の除電性能などの静
電気特性を簡便かつ正確に評価する構成からなる。すな
わち、本発明の静電気特性評価装置は、被測定物に所定
距離を隔てて対向配設する複数の表面電位計とから成る
表面電位検出手段と、被測定物の表面端部に接続される
電極と、該電極とアース間に接続するスイッチとから成
る放電手段と、該放電手段による被測定物に帯電した静
電気のアースへの放電時に前記複数の表面電位計によっ
て計測される各々の表面電位から相互間の電位差を検出
し、当該持続時間を演算する電位差持続時間検出回路
と、前記表面電位計の一方から出力される静電気の減衰
信号から放電時定数を計測する放電時定数検出回路と、
前記電位差持続時間および放電時定数の大きさを判定
し、被測定物の静電気特性として表示する表示回路とか
ら成る測定手段とを具備して成る。詳述すれば、本発明
装置は第1図に示すように、放電電極10とスイッチ11か
ら成る放電手段1によって被測定物3に帯電した静電気
を放電可能に構成してなる。該放電電極は一定面積の電
極面を有する導電部材から成り、被測定物上の任意の位
置にセット可能に構成されている。又被測定物を裏返せ
ば裏面から静電気を放電可能な構成である。
The apparatus for evaluating electrostatic characteristics of a charged body of the present invention measures the discharge state when static electricity charged on a measured object is forcibly discharged by a plurality of surface electrometers, and measures the discharge rate (time constant) of the static electricity. It is configured to easily and accurately evaluate the electrostatic characteristics such as the charge removal performance of the object to be measured from the magnitude and the magnitude of the potential difference obtained from the output differences of the surface electrometers. That is, the electrostatic characteristic evaluation apparatus of the present invention includes a surface potential detecting unit including a plurality of surface electrometers facing each other at a predetermined distance from the object to be measured, and an electrode connected to a surface end of the object to be measured. And a discharge means composed of a switch connected between the electrode and the ground, and from the respective surface potentials measured by the plurality of surface electrometers at the time of discharging the static electricity charged on the object to be measured by the discharge means to the ground. A potential difference duration detection circuit that detects a potential difference between each other and calculates the duration, and a discharge time constant detection circuit that measures a discharge time constant from an electrostatic decay signal output from one of the surface electrometers,
And a measuring circuit comprising a display circuit for judging the magnitude of the potential difference duration and the discharge time constant and displaying the static characteristic of the object to be measured. More specifically, as shown in FIG. 1, the device of the present invention is configured such that the static electricity charged on the DUT 3 can be discharged by the discharge means 1 including the discharge electrode 10 and the switch 11. The discharge electrode is composed of a conductive member having an electrode surface of a fixed area, and is configured to be settable at an arbitrary position on the object to be measured. Also, if the object to be measured is turned over, static electricity can be discharged from the back surface.

〔発明の作用・効果〕[Functions and effects of the invention]

本発明の静電気特性評価装置は静電気の放電時定数計
測が、被測定物表面上に接続する放電電極を任意の位置
にセットすることが可能であり、被測定物に対して、任
意な方向からその帯電した静電気を放電させる作用を奏
する。
The electrostatic characteristic evaluation apparatus of the present invention is capable of measuring the discharge time constant of static electricity, and setting the discharge electrode connected to the surface of the object to be measured at any position. It has the effect of discharging the charged static electricity.

これによって、被測定物の構造による局部的な静電気
分布や電荷の流れやすい放電経路などによって生じる放
電時定数変化を正確に測定できる効果を奏する。また被
測定物表面上の複数の位置に複数の表面電位計を配置す
ることにより、被測定物に帯電した静電気の放電時にお
ける、複数相互間の表面電位の電位差を実時間で計測す
る作用を行う。これによって、放電時の急峻な電位降下
の場合でも複数間の電位差を正確に検出でき、該電位差
の持続時間から被測定物の表面あるいは内部を通して移
動する電荷の移動速度を知ることができ、静電気の除電
性能を指示する有効な情報が得られるという従来では得
られない大きな効果を奏する。
As a result, there is an effect that it is possible to accurately measure a change in discharge time constant caused by a local static electricity distribution due to the structure of the object to be measured, a discharge path in which electric charges easily flow, or the like. Also, by arranging multiple surface electrometers at multiple positions on the surface of the object to be measured, it is possible to measure in real time the potential difference between the surface potentials of the multiple objects when the electrostatic charge on the object to be measured is discharged. To do. This makes it possible to accurately detect a plurality of potential differences even in the case of a sharp potential drop during discharge, and to know the moving speed of charges moving on the surface or inside of the DUT from the duration of the potential difference. A significant effect that cannot be obtained conventionally is obtained in that effective information indicating the static elimination performance of is obtained.

すなわち、上記構成からなる本発明の静電気特性評価
装置は、被測定物3上に表面電位検出手段2をセット
し、該被測定物3を帯電させた後、放電手段1によって
静電気をアースへ放電させる。該静電気の減衰状態は、
前記表面電位検出手段2で計測し、当該表面電位検出手
段2の出力信号の減衰特性から前記静電気の放電時定数
を測定装置5によって計測する。
That is, in the electrostatic characteristic evaluation apparatus of the present invention having the above configuration, the surface potential detecting means 2 is set on the object to be measured 3, the object to be measured 3 is charged, and then the static electricity is discharged to the ground by the discharging means 1. Let The state of decay of the static electricity is
The measurement is performed by the surface potential detecting means 2, and the discharge time constant of the static electricity is measured by the measuring device 5 from the attenuation characteristic of the output signal of the surface potential detecting means 2.

かかる構成において被測定物3への帯電手法は、コロ
ナ帯電法、摩擦帯電法、剥離帯電法などの手段が適用で
きる。
In this configuration, as a method of charging the DUT 3, a corona charging method, a friction charging method, a peeling charging method, or the like can be applied.

上記放電手段1、表面電位検出手段2、判定装置5か
ら成る静電気の放電時定数測定手段によれば、前記放電
手段1の被測定物3上へのセット位置を任意に変更でき
るため、被測定物3の構造、材質の不均一性などに基づ
く、放電時定数の差をあらゆる角度から計測することが
可能となり、従来技術では得ることができない格別顕著
な作用効果を奏する。次に表面電位検出手段2は、絶縁
台4上にセットする被測定物3に帯電した静電気を計測
するため、被測定物3面上の複数の例えば2点に任意距
離を隔てて第1の表面電位計20と第2の表面電位計21と
を設置する。該表面電位計20および21によって計測され
た表面電位信号は測定装置5に入力し、両信号の差を演
算せしめて、被測定物3面上2点間の電位差(第1図の
A点とB点)を測定する。
According to the electrostatic discharge time constant measuring means including the discharging means 1, the surface potential detecting means 2 and the determining device 5, the setting position of the discharging means 1 on the DUT 3 can be arbitrarily changed. It is possible to measure the difference in the discharge time constants from all angles based on the structure of the object 3, the non-uniformity of the material, and the like, and a particularly remarkable operation effect that cannot be obtained by the conventional technique is exhibited. Next, the surface potential detecting means 2 measures the static electricity charged on the object 3 to be measured set on the insulating table 4, and therefore, the first surface of the object 3 to be measured is separated by an arbitrary distance to a plurality of, for example, two points. A surface electrometer 20 and a second surface electrometer 21 are installed. The surface potential signals measured by the surface potential meters 20 and 21 are input to the measuring device 5 and the difference between the two signals is calculated to calculate the potential difference between the two points on the surface of the object 3 to be measured (point A in FIG. 1). Measure point B).

かかる構成によれば、前記放電手段1によって被測定
物3に帯電した静電気をアースに放電させると、被測定
物3上の電荷が放電電極側に向かって(A点からB点に
向かう)移動するため、A点とB点との2点間に生じる
電位差が検出される。この動作を第2図によって説明す
る。第2図において(A)、(B)、(C)は評価すべ
く被測定物3の種類を示す。又電圧信号Iは第1の表面
電位計20の出力、電圧信号IIは第2の表面電位計21の出
力、電圧信号IIIは測定装置5によって測定される前記
第1の表面電位計20と第2の表面電位計21との出力差を
示す。
According to this structure, when the static electricity charged on the DUT 3 is discharged to the ground by the discharging means 1, the charges on the DUT 3 move toward the discharge electrode side (from A point to B point). Therefore, the potential difference generated between the two points A and B is detected. This operation will be described with reference to FIG. In FIG. 2, (A), (B), and (C) show the types of the DUT 3 to be evaluated. The voltage signal I is the output of the first surface electrometer 20, the voltage signal II is the output of the second surface electrometer 21, and the voltage signal III is the first surface electrometer 20 and the first surface electrometer 20 measured by the measuring device 5. 2 shows the output difference with the surface electrometer 21.

第2図(A)は緩やかな放電時定数を呈する場合、第
2図(C)は急峻な放電時定数を呈する場合、第2図
(B)は両者の中間の放電時定数を呈する場合をそれぞ
れ示す。
FIG. 2 (A) shows a case where the discharge time constant is gentle, FIG. 2 (C) shows a case where the discharge time constant is steep, and FIG. 2 (B) shows a case where the discharge time constant is intermediate between the two. Shown respectively.

第2図(A)、(B)においては、被測定物3に帯電
した静電気を放電手段1によってアースへ放電させる
と、被測定物3面上の電荷が放電電極10に向かって移動
するため、A点に比べB点の電位が早く減衰(放電電極
10に近いため)する。従って、A点とB点との間には電
位差(第2図(A)、(B)、(C)中III)が生じ、
この電位差の発生する時期は、放電時定数が大きい程、
長く持続する。第2図(C)のように急峻な放電の場合
には、電位差も極く短時間出現する。
In FIGS. 2A and 2B, when the static electricity charged on the DUT 3 is discharged to the ground by the discharging means 1, the charge on the surface of the DUT 3 moves toward the discharge electrode 10. , The potential at point B decays faster than at point A (discharge electrode
Because it is close to 10.) Therefore, a potential difference (III in FIGS. 2 (A), (B), and (C)) occurs between points A and B,
The time when this potential difference occurs, the greater the discharge time constant,
Lasts a long time. In the case of a steep discharge as shown in FIG. 2 (C), the potential difference also appears for a very short time.

従ってこの電位差の持続時間が長い程、被測定物3上
の電荷の移動が遅いことを示す。これは被測定物3の表
面抵抗および体積抵抗が大きい程、電位差の持続時間が
長くなる実験的事実から、電位差の持続時間が長い被測
定物3(第2図(A)の場合)では、帯電した電荷の移
動がその高抵抗性によって遅くなることから、除電され
にくいと判断できる。すなわち電位差の持続時間が長い
場合は除電性能が悪いと判断できる。逆に被測定物3を
放電させた時、A点とB点の電位がほとんど同時に急峻
に減衰する(第2図(C))の場合は、被測定物3の電
荷がすばやく放電電極10に向かって移動するためであ
り、これは被測定物3の表面抵抗および体積抵抗が小さ
い程顕著になる。従って、この場合には電位差の出現時
間も極めて短くなることから、電位差の持続時間が短い
場合は、帯電した電荷が瞬時に放電される現象であり、
除電性能が良いと判断できる。以上の如く被測定物3に
帯電した静電気を放電手段1によって放電させ、該静電
気の減衰状態を被測定物面上の2点間で計測し、2点間
における電極差を計測し、その持続時間を判別すること
によって被測定物3、例えば帯電防止ファブリック等の
除電性能を高精度に測定できるという従来技術では期待
することができない大きな効果を奏する。
Therefore, the longer the duration of this potential difference, the slower the movement of the charges on the DUT 3. This is because from the experimental fact that the duration of the potential difference becomes longer as the surface resistance and volume resistance of the measurement object 3 become larger, the measurement object 3 (in the case of FIG. 2 (A)) having a long duration of the potential difference becomes Since the movement of the charged electric charge is delayed due to its high resistance, it can be determined that the electric charge is hardly removed. That is, if the duration of the potential difference is long, it can be determined that the static elimination performance is poor. On the contrary, when the DUT 3 is discharged, the electric potentials at the points A and B sharply decrease almost simultaneously (FIG. 2 (C)), the electric charge of the DUT 3 quickly flows to the discharge electrode 10. This is because the surface resistance and volume resistance of the DUT 3 become smaller as the surface resistance and volume resistance of the DUT 3 become smaller. Therefore, in this case, since the appearance time of the potential difference becomes extremely short, if the duration of the potential difference is short, it is a phenomenon that the charged charge is instantly discharged,
It can be judged that the static elimination performance is good. As described above, the static electricity charged on the object to be measured 3 is discharged by the discharging means 1, the decay state of the static electricity is measured between two points on the surface of the object to be measured, the electrode difference between the two points is measured, and the continuation is maintained. By discriminating the time, there is a great effect that cannot be expected in the conventional technology that the static elimination performance of the DUT 3, for example, the antistatic fabric can be measured with high accuracy.

〔実施例〕〔Example〕

以下本発明の代表的な実施例を第3図、第4図に基づ
き説明する。
A typical embodiment of the present invention will be described below with reference to FIGS. 3 and 4.

本実施例の帯電体の静電気特性評価装置は、放電手段
1と表面電位検出手段2と測定装置5とから成る。放電
手段1はアクリルなどの絶縁材から構成した絶縁台4上
にセットされる被測定物3の表面の一端に接触、接続す
る導電材から成る一定面積を有する放電電極10と、一端
が該放電電極10に接続され、他端がアースに接続されて
なり、測定装置5からの付勢信号によって動作すべく高
耐電圧のスイッチ11とから成る。かかる放電手段1は、
放電電極10が被測定物3上の任意の位置にセットするこ
とが可能であり、被測定物3に帯電した静電気を任意位
置からアースに放電可能に構成される。
The apparatus for evaluating electrostatic characteristics of a charged body according to this embodiment includes a discharging unit 1, a surface potential detecting unit 2 and a measuring unit 5. The discharge means 1 is a discharge electrode 10 having a certain area made of a conductive material, which is in contact with and connected to one end of the surface of the DUT 3 set on an insulating base 4 made of an insulating material such as acrylic, and one end of the discharge electrode 10. It is connected to the electrode 10 and the other end is connected to the ground, and comprises a switch 11 having a high withstand voltage so as to be operated by an energizing signal from the measuring device 5. The discharging means 1 is
The discharge electrode 10 can be set at any position on the DUT 3, and the static electricity charged on the DUT 3 can be discharged from any position to the ground.

更に、スイッチ11は接点耐圧を十分高くした高絶縁性
のリレーを用いることにより、被測定物3の静電気がス
イッチ11からリークすることなく、長期間、安定に静電
気を保持できると共に、測定装置5からの付勢信号によ
って、任意タイミングで自動的に静電気を放電させる動
作ができる。
Further, the switch 11 uses a highly insulating relay having a sufficiently high contact breakdown voltage, so that the static electricity of the DUT 3 can be stably held for a long period of time without leaking from the switch 11, and the measuring device 5 can be used. A static electricity can be automatically discharged at an arbitrary timing by an energizing signal from.

次に表面電位検出手段2は、第1の表面電位計20と第
2の表面電位計21とから成り、被測定物3の表面空間上
の2点位置に任意距離を隔てて、それぞれ配置する。従
って第1の表面電位計20は被測定物3表面のA点周辺、
第2の表面電位計21はB点周辺の表面電位が計測可能で
ある。
Next, the surface potential detecting means 2 is composed of a first surface potential meter 20 and a second surface potential meter 21, and is arranged at two points on the surface space of the DUT 3 at arbitrary distances. . Therefore, the first surface electrometer 20 is around the point A on the surface of the DUT 3,
The second surface potential meter 21 can measure the surface potential around the point B.

該表面電位検出手段2の出力は測定装置5に入力され
て、被測定物3に帯電した静電気を前記放電手段1によ
って放電させた時の静電気の減衰状態から、静電気の放
電時定数およびA点とB点間における電位差が計測され
る。測定装置5は、前記第1の表面電位計20と第2の表
面電位計21の出力が入力され、その差を演算せしめる差
動演算回路51と、該差動演算回路51の出力を受けて、前
記被測定物3上のA点とB点との電位差として計測し、
該電位差信号の持続時間を検出する電位差持続時間検出
回路52と、前記表面電位計20もしくは21の出力を受け
て、被測定物3の静電気が一定電位以下になったことを
判別するコンパレータ53と該コンパレータ53から出力さ
れる信号を受けて、前記静電気の放電時定数を検出する
放電時定数検出回路54と、前記電位差持続時間検出回路
52および前記放電時定数検出回路54とから出力される信
号を受けて、被測定物3の静電気の除電性能を評価すべ
く結果を判定、表示する表示回路55と、前記放電手段1
を構成するスイッチ11を付勢すると共に前記放電時定数
検出回路54の信号処理タイミングを制御する制御回路56
とから構成される。
The output of the surface potential detecting means 2 is input to the measuring device 5, and the static electricity discharge time constant and the point A are calculated from the static electricity decay state when the static electricity charged on the DUT 3 is discharged by the discharging means 1. And the potential difference between point B is measured. The measuring device 5 receives the outputs of the first surface electrometer 20 and the second surface electrometer 21 and receives a differential operation circuit 51 for calculating the difference between them and an output of the differential operation circuit 51. , Is measured as a potential difference between points A and B on the DUT 3,
A potential difference duration detection circuit 52 for detecting the duration of the potential difference signal, and a comparator 53 for receiving the output of the surface electrometer 20 or 21 and determining whether the static electricity of the DUT 3 has become a certain potential or less. A discharge time constant detection circuit 54 that receives the signal output from the comparator 53 and detects the discharge time constant of the static electricity, and the potential difference duration detection circuit
A display circuit 55 that receives and outputs signals output from the discharge time constant detection circuit 54 and the discharge time constant detection circuit 54 to judge and display the result in order to evaluate the static elimination performance of the DUT 3;
Control circuit 56 for energizing the switch 11 constituting the above and controlling the signal processing timing of the discharge time constant detection circuit 54.
It is composed of

以上の構成から成る測定装置5の作用効果を第4図
(A)〜(G)に示すタイムチャートによって説明す
る。
The operation and effect of the measuring device 5 having the above configuration will be described with reference to the time charts shown in FIGS.

被測定物3に帯電した静電気を前記放電手段1によっ
てアースへ放電させた時の被測定物3の表面電位の減衰
状態は前記表面電位検出手段2によって計測される。該
検出手段2の第1の表面電位計20によって検出される電
位信号V1(第4図(A))は差動演算回路51の一方の入
力端子に入力され、更に第2の表面電位計21によって検
出される電位信号V2(第4図(B))は、前記差動演算
回路51の他方の入力端子に入力され、両信号の電位差が
演算される。該電位差信号ΔV(第4図(F))は、次
に電位差持続時間検出回路52に入力し、前記電位差信号
ΔVを基準値etによって判別することにより、該電位差
信号の持続時間tに比例した時間信号t(第4図
(G))に変換する。該持続時間信号tは、表示回路55
によって、電位差ΔVの持続時間信号tの大きさを判定
し、被測定物3の静電気に対する除電性能を示す量とし
て表示する。
The decay state of the surface potential of the DUT 3 when the static electricity charged on the DUT 3 is discharged to the ground by the discharging means 1 is measured by the surface potential detecting means 2. The potential signal V 1 (FIG. 4 (A)) detected by the first surface electrometer 20 of the detecting means 2 is input to one input terminal of the differential operation circuit 51, and further the second surface electrometer. The potential signal V 2 (FIG. 4 (B)) detected by 21 is input to the other input terminal of the differential operation circuit 51, and the potential difference between both signals is calculated. The difference signal [Delta] V (FIG. 4 (F)) is then input to the potential difference duration detection circuit 52, by determining the difference signal [Delta] V by the reference value e t, proportional to the duration t of the potential difference signal It is converted into the time signal t (FIG. 4 (G)). The duration signal t is displayed by the display circuit 55.
Then, the magnitude of the duration signal t of the potential difference ΔV is determined and displayed as an amount indicating the static elimination performance of the DUT 3 against static electricity.

次に第2の表面電位計21によって検出される電位信号
V2(第4図(B))はコンパレータ53に入力する。該コ
ンパレータ53は、電位信号V2が一定基準以下に減衰する
時間を判別するものであり、前記V2が基準値e1以下に達
するとコンパレータ53が動作し、判定信号(第4図
(D))を出力する。該判定信号は、前記放電手段1を
動作すべく制御回路56から出力されるスタート信号(第
4図(C))との作用により前記電位信号V2の放電時定
数τに比例した放電時定数信号(第4図(E))に変換
する。該放電時定数信号は表示回路55に入力し、放電時
定数として表示すと共にその大きさを判定して、被測定
物3の静電気に対する除電性能を表す値として表示す
る。
Next, the potential signal detected by the second surface electrometer 21
V 2 (FIG. 4 (B)) is input to the comparator 53. The comparator 53 determines the time when the potential signal V 2 decays below a certain reference, and when the V 2 reaches a reference value e 1 or below, the comparator 53 operates and a determination signal (see FIG. )) Is output. The judgment signal is a discharge time constant proportional to the discharge time constant τ of the potential signal V 2 by the action of the start signal (FIG. 4 (C)) output from the control circuit 56 to operate the discharge means 1. Signal (FIG. 4 (E)). The discharge time constant signal is input to the display circuit 55, displayed as a discharge time constant, and its magnitude is determined and displayed as a value representing the static elimination performance of the DUT 3 against static electricity.

【図面の簡単な説明】[Brief description of drawings]

第1図は本発明の静電気特性評価装置の概略を示す概要
図、第2図(A)〜(C)は、本発明装置の動作内容を
それぞれ示す線図、第3図は本発明の一実施例装置を示
す線図、第4図(A)〜(G)は本発明の一実施例装置
の動作内容をそれぞれ示す線図である。 図中 1……放電手段 2……表面電位検出手段 3……被測定物 4……絶縁台 5……測定装置 20……第1の表面電位計 21……第2の表面電位計
FIG. 1 is a schematic diagram showing an outline of the electrostatic characteristic evaluation device of the present invention, FIGS. 2 (A) to (C) are diagrams showing the operation contents of the device of the present invention, and FIG. FIG. 4A is a diagram showing an apparatus according to the embodiment, and FIGS. 4A to 4G are diagrams showing the operation contents of the apparatus according to the embodiment of the present invention. In the figure 1 ... Discharging means 2 ... Surface potential detecting means 3 ... Object to be measured 4 ... Insulation stand 5 ... Measuring device 20 ... First surface electrometer 21 ... Second surface electrometer

───────────────────────────────────────────────────── フロントページの続き (72)発明者 梅本 芳朗 愛知県豊田市トヨタ町1番地 トヨタ自 動車株式会社内 (72)発明者 大野 秀樹 愛知県豊田市トヨタ町1番地 トヨタ自 動車株式会社内 審査官 小川 浩史 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Yoshiro Umemoto 1 Toyota Town, Toyota City, Aichi Prefecture, Toyota Motor Co., Ltd. (72) Inventor Hideki Ohno 1 Toyota Town, Aichi Prefecture, Toyota Motor Company, Ltd. Hiroshi Ogawa

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】被測定物に所定距離を隔てて対向配設する
複数の表面電位計から成る表面電位検出手段と、被測定
物の表面端部に接続される電極と、該電極とアース間に
接続するスイッチとから成る放電手段と、該放電手段に
よる被測定物に帯電した静電気のアースへの放電時に前
記複数の表面電位計によつて計測される各々の表面電位
から相互間の電位差を検出し、当該持続時間を演算する
電位差持続時間検出回路と、前記表面電位計の一方から
出力される静電気の減衰信号から放電時定数を計測する
放電時定数検出回路と、前記電位差持続時間および放電
時定数の大きさを判定し、被測定物の静電気特性として
表示する表示回路とから成る測定手段とを具備したこと
を特徴とする静電気特性評価装置。
1. A surface potential detecting means composed of a plurality of surface electrometers facing each other at a predetermined distance from an object to be measured, an electrode connected to a surface end of the object to be measured, and a gap between the electrode and the ground. And a discharge means composed of a switch connected to the discharge means, and a potential difference between the respective surface potentials measured by the plurality of surface electrometers at the time of discharging the static electricity charged on the object to be measured by the discharge means to the ground. A potential difference duration detection circuit that detects and calculates the duration, a discharge time constant detection circuit that measures a discharge time constant from an electrostatic decay signal output from one of the surface electrometers, the potential difference duration and discharge An electrostatic characteristic evaluation apparatus comprising: a measuring circuit including a display circuit that determines the magnitude of a time constant and displays the electrostatic characteristic of an object to be measured.
JP1049483A 1989-03-01 1989-03-01 Electrostatic characteristic evaluation device Expired - Fee Related JP2557704B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1049483A JP2557704B2 (en) 1989-03-01 1989-03-01 Electrostatic characteristic evaluation device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1049483A JP2557704B2 (en) 1989-03-01 1989-03-01 Electrostatic characteristic evaluation device

Publications (2)

Publication Number Publication Date
JPH0328776A JPH0328776A (en) 1991-02-06
JP2557704B2 true JP2557704B2 (en) 1996-11-27

Family

ID=12832405

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1049483A Expired - Fee Related JP2557704B2 (en) 1989-03-01 1989-03-01 Electrostatic characteristic evaluation device

Country Status (1)

Country Link
JP (1) JP2557704B2 (en)

Families Citing this family (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002239435A (en) * 2001-02-16 2002-08-27 Matsushita Electric Ind Co Ltd Apparatus and method for applying viscous material
JP2004358679A (en) * 2003-06-02 2004-12-24 Yokohama Rubber Co Ltd:The Method and device for detecting earthing effect of tire
JP2009053074A (en) * 2007-08-28 2009-03-12 Shishido Seidenki Kk Electric field detection device
JP5510629B2 (en) * 2009-02-20 2014-06-04 国立大学法人山形大学 Charge transfer rate measuring device and method, surface resistance measuring device and method, and program for them
JP5531869B2 (en) * 2010-09-10 2014-06-25 株式会社村田製作所 Discharge characteristic test apparatus and discharge characteristic test method
JP5679858B2 (en) * 2011-02-22 2015-03-04 ホーヤ レンズ マニュファクチャリング フィリピン インク Spectacle inspection jig for spectacle lens and electrification inspection method for spectacle lens
JP6354077B2 (en) * 2013-12-27 2018-07-11 国立大学法人山形大学 Paint dryness measuring device
JPWO2017168608A1 (en) * 2016-03-30 2018-12-27 株式会社日立システムズ Non-contact voltage measuring device and non-contact voltage measuring method
CN112986761B (en) * 2021-02-08 2022-08-16 苏州天华超净科技股份有限公司 Method for monitoring working performance of electrostatic eliminator
CN114034943B (en) * 2021-11-09 2024-04-05 华北电力大学 Surface potential attenuation measuring device and method and charge transport process determining method

Also Published As

Publication number Publication date
JPH0328776A (en) 1991-02-06

Similar Documents

Publication Publication Date Title
JP2557704B2 (en) Electrostatic characteristic evaluation device
US4914394A (en) Pocket-size time domain reflectometer
US4575580A (en) Data input device with a circuit responsive to stylus up/down position
US2856582A (en) Method and apparatus for measuring thickness
US5455507A (en) Method and apparatus for detecting leaks in electrically-insulative protective articles such as condoms, surgical gloves and the like using gaseous electrostatic ions
US5272817A (en) Signal conditioning circuit for trigger probe
US3406334A (en) Apparatus for testing electrostatic copy material
US5359282A (en) Plasma diagnosing apparatus
Dawson The lifetime of positive streamers in a pulsed point-to-plane gap in atmospheric air
US7710205B2 (en) Capacitor detection by phase shift
AU715105B2 (en) Electronic signal measurement apparatus and method for the acquisition and display of short-duration analog signal events
Blacker et al. Electrostatic charge occurrence, significance and measurement
JPH11211770A (en) Static electricity evaluation device
US3790887A (en) Amplifying and holding measurement circuit
US4231258A (en) Method and apparatus for detecting foreign matters in gas sealed electric apparatus
JPS5763461A (en) Device for testing watermeter
JPH03154879A (en) Substrate inspecting device
US5016136A (en) Charge build-up and decay monitor
JPS6457276A (en) Image forming device
Chubb et al. Comparative studies on methods of charge decay measurement
JPH0827307B2 (en) Printed wiring board test equipment
SU1434348A1 (en) Method of electric resistance flaw detection in conducting media
JPS6228654A (en) Detection of crack
KR0122101B1 (en) Electrolytic condenser checking system
KR840004186A (en) Plating control inspection method and device

Legal Events

Date Code Title Description
R250 Receipt of annual fees

Free format text: JAPANESE INTERMEDIATE CODE: R250

LAPS Cancellation because of no payment of annual fees