JPH09178590A - Method for deciding go/no-go of pressure sensor - Google Patents

Method for deciding go/no-go of pressure sensor

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Publication number
JPH09178590A
JPH09178590A JP35094895A JP35094895A JPH09178590A JP H09178590 A JPH09178590 A JP H09178590A JP 35094895 A JP35094895 A JP 35094895A JP 35094895 A JP35094895 A JP 35094895A JP H09178590 A JPH09178590 A JP H09178590A
Authority
JP
Japan
Prior art keywords
vacuum
voltage
pressure
pressure sensor
sensor
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.)
Pending
Application number
JP35094895A
Other languages
Japanese (ja)
Inventor
Masahiro Ueda
上田正紘
Atsuo Irisa
入佐厚生
Tomio Matsui
松井富雄
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.)
Hokkei Kogyo KK
Original Assignee
Hokkei Kogyo KK
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 Hokkei Kogyo KK filed Critical Hokkei Kogyo KK
Priority to JP35094895A priority Critical patent/JPH09178590A/en
Publication of JPH09178590A publication Critical patent/JPH09178590A/en
Pending legal-status Critical Current

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Abstract

PROBLEM TO BE SOLVED: To provide a method for estimating the vacuum leakage and electric circuit defect of a strain gauge type pressure sensor being employed as a vacuum sensor accurately in safety without utilizing radioactivity and without causing any pollution over a wide range of discharge and electric output characteristics. SOLUTION: Upon elapse of about 10 days after manufacture of a sensor, a DC 600V voltage is applied between a metal case 6 and the terminal where all electrodes 2 are short-circuited. If a discharge current flows, it means vacuum leakage at a rate higher than maximum allowable rate and thereby the sensor is rejected otherwise a DC 6V voltage is applied to the electrode 2 and the output voltage is recorded. Upon elapse of another 10 days, output voltage is measured and if the voltage difference is higher than several mV, a decision is made that the maximum allowable vacuum leakage rate is exceeded and the sensor is rejected.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【発明の属する技術分野】本発明は、歪みゲージ式の圧
力センサーの真空漏れについての良否判定方法に関す
る。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a pass / fail judgment method for vacuum leakage of a strain gauge type pressure sensor.

【0002】[0002]

【従来の技術及び発明が解決しようとする課題】歪みゲ
ージ式の圧力センサーは、例えば自動車用のエンジンの
高効率化等のための真空センサーとして必要不可欠のも
のである。通常のこの種の圧力センサーは、内部の高真
空領域と外部からの圧力導入管との間の圧力差を、両者
の間に真空的に絶縁して設置した圧電素子により検出
し、検出値を電気信号として増幅して取り出している。
製造時の内部真空度は通常6.7Pa(0.05Tor
r)以下であり、真空センサーとしての耐久年数は20
年以上である。即ち、実用化されているこの種の圧力セ
ンサーの最大許容真空漏れ率としては、1.0×10-5
Pa・cc/sec以下が必要であるといわれている。
2. Description of the Related Art A strain gauge type pressure sensor is indispensable as a vacuum sensor for improving the efficiency of an automobile engine, for example. A normal pressure sensor of this type detects the pressure difference between the high vacuum region inside and the pressure introducing pipe from the outside by means of a piezoelectric element that is vacuum insulated between the two and detects the detected value. It is amplified and taken out as an electric signal.
The internal vacuum degree during manufacturing is usually 6.7 Pa (0.05 Tor)
r) or less, and the durability as a vacuum sensor is 20
More than a year. That is, the maximum permissible vacuum leak rate of this type of pressure sensor that has been put to practical use is 1.0 × 10 −5.
It is said that it is necessary to have Pa · cc / sec or less.

【0003】このセンサー構造では、内部の真空度があ
る値まで低下すると圧電素子の出力電気信号が外部から
の圧力変化に比例しなくなるので、真空漏れは圧力セン
サーとしては致命傷となる。このため種々の検査が行わ
れているが、現行の一般的な検査方法は、圧力センサー
を放射性物質の加圧釜中に数日間封入し、真空漏れが生
じていれば放射能ガスを吸引してしまうので、それを取
り出して放射能強度をガイガーカウンター等で測定し、
良否や真空漏れ率を判定するというものである。
In this sensor structure, when the internal vacuum degree drops to a certain value, the output electric signal of the piezoelectric element becomes non-proportional to the pressure change from the outside, so that the vacuum leakage is fatal to the pressure sensor. For this reason, various inspections have been carried out, but the current general inspection method is to seal the pressure sensor in a pressurized vessel of radioactive material for several days, and if a vacuum leak occurs, suck the radioactive gas. Since it will be stored, take out it and measure the radioactivity intensity with a Geiger counter etc.
The quality is determined and the vacuum leakage rate is determined.

【0004】しかしながら上述の従来の良否判定方法で
は放射能汚染による公害という問題が付きまとうという
問題がある。即ち、放射能物質の取り扱いが大変困難
で、作業環境、作業者の就労性が大変に悪い。本発明は
このような従来の問題点に鑑み、簡易かつ安全で、しか
も正確、無公害かつ経済的な圧力センサーの良否判定方
法を提供することを目的とする。
However, the above-mentioned conventional quality determination method has a problem of pollution due to radioactive contamination. That is, it is very difficult to handle radioactive substances, and the work environment and the workability of workers are very poor. The present invention has been made in view of such conventional problems, and an object of the present invention is to provide a simple, safe, accurate, pollution-free and economical method for determining the quality of a pressure sensor.

【0005】また、たとえ圧力センサー内部の真空度が
保たれていても、電気回路的な欠陥が存在していて不良
品である場合もある。従って本発明は、電気回路に欠陥
があるか否かを簡易かつ早く検査できる圧力センサーの
良否判定方法を提供することをも目的とする。
Further, even if the vacuum degree inside the pressure sensor is maintained, there are cases in which there is an electric circuit defect and the product is defective. Accordingly, it is another object of the present invention to provide a method for determining the quality of a pressure sensor, which can easily and quickly inspect whether or not there is a defect in an electric circuit.

【0006】[0006]

【課題を解決するための手段】本発明は真空の漏れ率の
ごく小さい領域では放電現象によって、それ以上の漏れ
率の大きい領域では電気的な出力信号から推定する方法
を提案する。
The present invention proposes a method of estimating from a discharge phenomenon in a region where the leak rate of a vacuum is very small, and from an electrical output signal in a region where the leak rate is higher than that.

【0007】本発明に係る圧力センサーの良否判定方法
は、上記目的を達成するために、ケース内の真空度と圧
力導入部に印加される圧力との差から生じる歪電圧によ
って圧力を測定する歪みゲージ式の圧力センサーについ
て真空漏れの良否を判定する方法であって、センサー製
造日から所定時間経過後に、すべての電極を短絡した端
子と上記ケースとの間に所定値の直流高電圧を印加し、
放電電流が流れれば真空漏れが生じているものとして不
良品と判断し、放電が生じない場合には、上記電極に所
定値の直流バイアス電圧を印加してその出力電圧を記録
しておき、さらに所定時間経過後に再び全く同じ値の直
流バイアス電圧を印加して出力電圧を測定し、測定した
電圧差が所定値以上であれば真空漏れが生じているもの
として不良品と判断することを特徴とする。
In order to achieve the above-mentioned object, the method for judging the quality of a pressure sensor according to the present invention is a strain for measuring the pressure by a strain voltage generated from the difference between the degree of vacuum in the case and the pressure applied to the pressure introducing portion. This is a method for judging the quality of vacuum leakage of a gauge type pressure sensor, and after a predetermined time has elapsed from the sensor manufacturing date, a high DC voltage of a predetermined value is applied between the terminals with all the electrodes short-circuited and the case. ,
If a discharge current flows, it is determined that a vacuum leak has occurred and the product is defective.If no discharge occurs, a DC bias voltage of a predetermined value is applied to the electrode and the output voltage is recorded. Further, after a lapse of a predetermined time, a DC bias voltage of exactly the same value is applied again to measure the output voltage, and if the measured voltage difference is equal to or more than a predetermined value, it is determined that a vacuum leak has occurred and the product is defective. And

【0008】[0008]

【発明の実施の形態】まず本発明の原理を説明すると、
放電現象を利用する真空漏れ率の測定について説明す
る。電場が一様で気体の温度、湿度が一定ならば、火花
放電を起こすのに必要な最小電圧を、電極間距離と気体
の圧力との積の関数として定められるというパッシェン
の法則(Paschen's Law )によって、真空圧の違いによ
って生じる放電開始電圧または放電電流からその真空圧
P1が推定できるので、圧力センサーに封じ込んだとき
の真空圧P0との差がわかり、したがって封じ込み時か
ら測定時までの時間Tからその期間における平均的な真
空漏れ率Rが下記の数式1により概算できる。
BEST MODE FOR CARRYING OUT THE INVENTION First, the principle of the present invention will be described.
The measurement of the vacuum leakage rate using the discharge phenomenon will be described. Paschen's Law, which states that the minimum voltage required to cause a spark discharge is defined as a function of the product of the distance between electrodes and the pressure of gas if the electric field is uniform and the temperature and humidity of gas are constant. Since the vacuum pressure P1 can be estimated from the discharge start voltage or the discharge current caused by the difference in the vacuum pressure, the difference with the vacuum pressure P0 when the pressure sensor is sealed is known, and therefore, from the time of sealing to the time of measurement. From time T, the average vacuum leak rate R in that period can be roughly calculated by the following formula 1.

【数1】R=(P1−P0)・v/T [Pa・
cc/sec] 式中のvは圧力センサーの内部容積である。
[Formula 1] R = (P1-P0) · v / T [Pa ·
cc / sec] In the formula, v is the internal volume of the pressure sensor.

【0009】真空封じ込み時の内部圧力は、上述のよう
に例えば6.7Paとかなりの高真空になっているの
で、センサーの金属ケース間と各電極間に適当な電圧、
たとえば数百Vを印加しても放電は生じないが、真空漏
れが生じて真空度が適度に低下しているとパッシェンの
法則に従った放電が生じる。この時の放電電圧または放
電電流から真空度が推定できる。
Since the internal pressure at the time of vacuum containment is a considerably high vacuum, for example, 6.7 Pa as described above, an appropriate voltage between the metal case of the sensor and each electrode,
For example, even if several hundreds V is applied, no discharge occurs, but if vacuum leakage occurs and the degree of vacuum is appropriately lowered, discharge according to Paschen's law occurs. The degree of vacuum can be estimated from the discharge voltage or discharge current at this time.

【0010】もちろん実際の圧力センサ−内の真空度を
直接測定することは出来ないので、図1(A)、(B)
に示す構造の圧力センサー1について、図2に示すよう
な真空装置及び電圧印加系を接続して測定を行う。
Of course, it is not possible to directly measure the degree of vacuum inside the actual pressure sensor, and therefore, as shown in FIGS. 1 (A) and 1 (B).
With respect to the pressure sensor 1 having the structure shown in FIG. 2, a vacuum device and a voltage application system as shown in FIG.

【0011】まず圧力センサー1は、ベース1aに複数
本の電極2・・・と圧力導入管3を互いに電気的に絶縁
して設け、圧力導入管3の先端に金属ダイアフラム4を
取り付け、ダイアフラム面上の圧電素子5・・・を設
け、圧電素子5と電極2との間に配線し、それらの上部
を金属ケース6で覆って構成してある。そして、このよ
うな圧力センサー1の圧力導入管3とロータリーポンプ
7との間に配管8を配して圧力を印加可能とし、配管8
の途中にピラニー真空計9と圧力調整弁10を接続する
とともに、圧力センサー1の複数のすべての電極2の端
子を短絡し、電圧印加用の電源11と電圧計12を接続
する。
First, in the pressure sensor 1, a plurality of electrodes 2, ... And a pressure introducing pipe 3 are provided on a base 1a so as to be electrically insulated from each other, and a metal diaphragm 4 is attached to the tip of the pressure introducing pipe 3 to form a diaphragm surface. The upper piezoelectric element 5 is provided, wiring is provided between the piezoelectric element 5 and the electrode 2, and the upper portions thereof are covered with the metal case 6. Then, a pipe 8 is arranged between the pressure introducing pipe 3 and the rotary pump 7 of the pressure sensor 1 as described above so that pressure can be applied.
In the middle of, the Pirani vacuum gauge 9 and the pressure adjusting valve 10 are connected, the terminals of all the electrodes 2 of the pressure sensor 1 are short-circuited, and the power supply 11 for voltage application and the voltmeter 12 are connected.

【0012】このような系において、電源11によって
数百ボルト程度の適当な値の放電電圧を印加すると、圧
力センサー1内の真空度がある適当な範囲内では適度の
大きさの放電電圧で放電が生じ、その放電電流から真空
度が推定できる。しかし、上記範囲よりも高真空度側あ
るいは低真空度側では放電が生じないため、圧力センサ
ー1の内の真空度を判定できない。
In such a system, when a discharge voltage of an appropriate value of about several hundreds of volts is applied by the power supply 11, the pressure sensor 1 is discharged with a discharge voltage of an appropriate magnitude within a certain range of vacuum. Occurs, and the degree of vacuum can be estimated from the discharge current. However, since the discharge does not occur on the higher or lower vacuum side than the above range, the degree of vacuum in the pressure sensor 1 cannot be determined.

【0013】即ち、放電が生じないのはその圧力センサ
ー1が良品であって内部が所定の真空度に保たれている
か、あるいは放電が生じなくても所定の真空漏れ率範囲
を超える速さで真空漏れが生じているかである。そこ
で、圧力センサー1の電極2・・・に数V程度の直流電
圧を印加してその出力電圧を記録しておき、さらに10
日間程度放置した後に再び出力電圧を測定し、その電圧
差が数mV以上あれば、最大許容真空漏れ率を大きく超
える速さで漏れており不良品であると判断できる。この
場合の出力電圧は、図4のごとく、圧力センサー1の内
部と外部の圧力差(外部圧−内部圧)に比例するので、
圧力導入管3から印加する圧力はこの差が常に正となる
ように設定する。
That is, the discharge does not occur if the pressure sensor 1 is a good product and the inside is kept at a predetermined vacuum degree, or even if the discharge does not occur at a speed exceeding a predetermined vacuum leakage rate range. Is there a vacuum leak? Therefore, a direct current voltage of about several volts is applied to the electrodes 2 of the pressure sensor 1, and the output voltage is recorded.
The output voltage is measured again after being left for about a day, and if the voltage difference is several mV or more, it can be determined that the product is defective because it leaks at a speed that greatly exceeds the maximum allowable vacuum leak rate. The output voltage in this case is proportional to the pressure difference between the inside and the outside of the pressure sensor 1 (external pressure-internal pressure) as shown in FIG.
The pressure applied from the pressure introducing pipe 3 is set so that this difference is always positive.

【0014】[0014]

【実施例】次に本発明の実施例を、圧力センサー1内の
圧力P1を変化させたときの放電開始電圧Vdおよび放
電電流Idの測定結果を示す図3と、再び図2をも参照
して説明する。放電電圧の最大値を600Vとし(別途
の試験により圧力センサー1内に内蔵する歪電圧増幅用
のIC回路が破壊されるのは放電電圧が1000V程度
であったので、安全性を見込んでこのように設定し
た。)、本発明を実施したところ、放電が生じる圧力範
囲は約20Pa〜800Paであった。この範囲では放
電電流値からそのときの圧力P1がほぼ正確にわかり、
既に述べたようにパッシェンの法則に基づいて圧力セン
サー1内の真空度を推定できた。
EXAMPLE An example of the present invention will now be described with reference to FIG. 3 showing the measurement results of the discharge start voltage Vd and the discharge current Id when the pressure P1 in the pressure sensor 1 is changed, and again with reference to FIG. Explain. The maximum value of the discharge voltage is set to 600V (The IC circuit for amplifying the strain voltage built in the pressure sensor 1 is destroyed by a separate test because the discharge voltage is about 1000V. When the present invention was carried out, the pressure range in which discharge occurred was about 20 Pa to 800 Pa. In this range, the pressure P1 at that time can be known almost accurately from the discharge current value,
As described above, the degree of vacuum in the pressure sensor 1 could be estimated based on Paschen's law.

【0015】たとえば圧力センサー1の真空封じ込み時
圧力P0=6.7Pa、封じ込み時から10日後の圧力
P1=20Pa、センサー内部容積v=0.5ccとす
れば、上述の数式1より、真空漏れ率はR=0.77×
10-5(Pa・cc/sec)となり、この場合は辛う
じて最大許容真空漏れ率Rm以下となる。逆に、P1=
800PaとすればR=4.6×10-4(Pa・cc/
sec)となり、最大許容真空漏れ率Rmの約50倍の
速さで真空漏れが生じていることになる。
For example, assuming that the pressure P0 of the pressure sensor 1 during vacuum containment is P0 = 6.7 Pa, the pressure 10 days after the containment is P1 = 20 Pa, and the internal volume v of the sensor is v = 0.5 cc, the vacuum is calculated from the above formula 1. Leak rate is R = 0.77 ×
It becomes 10 −5 (Pa · cc / sec), and in this case, it is barely less than the maximum allowable vacuum leakage rate Rm. Conversely, P1 =
If it is 800 Pa, R = 4.6 × 10 −4 (Pa · cc /
sec), which means that the vacuum leak occurs at a speed of about 50 times the maximum allowable vacuum leak rate Rm.

【0016】一方、上述のように20Pa以下の圧力及
び800Pa以上の圧力範囲では放電が生じないので、
圧力センサー1内の真空度が推定できない。そこで、図
2のシステムにおいて電源11により直流バイアス電圧
Vcc=6Vを印加してピラニー真空計9の測定端子圧
Pxを徐々に増加させながら電圧計12により出力電圧
Voを測定した。図4にその測定結果を示す。同図には
良品の圧力センサーにおいて測定端子圧力Pxを変化さ
せたときの電気出力を示す。
On the other hand, as described above, since discharge does not occur in the pressure range of 20 Pa or less and the pressure range of 800 Pa or more,
The degree of vacuum in the pressure sensor 1 cannot be estimated. Therefore, in the system of FIG. 2, the output voltage Vo was measured by the voltmeter 12 while applying the DC bias voltage Vcc = 6V from the power supply 11 to gradually increase the measurement terminal pressure Px of the Pirani vacuum gauge 9. The measurement result is shown in FIG. In the same figure, the electric output when the measuring terminal pressure Px is changed in the pressure sensor of the non-defective product is shown.

【0017】不良品の圧力センサーの出力は、圧力Px
の変化にかかわらず直流バイアス電圧に近い一定値とな
っているのに対し、良品の圧力センサー出力は、大気圧
近く(4×104 Pa)まではバイアス電圧の1〜2割
程度の小さい値ながら、圧力増加とともに僅かに増加
し、大気圧に近付くと急激に直流バイアス電圧値まで増
加している。この圧力増加は圧力センサーの内部圧P1
が高真空となっているので、実際には圧力差(Px−P
1)の増加である。外部からの圧力導入パイプ3に加え
る圧力Pxを一定にしておけば、この僅かな電圧変化は
センサー内部の圧力変化P1によって生じるので、上述
の数式1から真空漏れ率が推定できる。前述のように、
真空漏れが大きくて放電が生じないとすれば、それは少
なくても最大許容真空漏れ率の50倍程度以上で、10
日間も放置すれば1000Pa以上の圧力増加があり
(たとえば50倍の速さで漏れているとすると、10日
後の圧力は1600Pa(=12Torr)とな
る。)、この圧力増加に対する電圧変化は数mVとなっ
て十分に読み取れ、この電圧増加を測定することによっ
てその間での圧力変化、即ち真空漏れ率を数式1で概算
することができる。
The output of the defective pressure sensor is the pressure Px.
Is a constant value close to the DC bias voltage regardless of the change of, the output of the pressure sensor of a good product is a small value of about 10 to 20% of the bias voltage up to near atmospheric pressure (4 × 10 4 Pa). However, it increases slightly as the pressure increases, and rapidly increases to the DC bias voltage value when approaching atmospheric pressure. This pressure increase is due to the internal pressure P1 of the pressure sensor.
Is a high vacuum, the pressure difference (Px-P
1) increase. If the pressure Px applied to the pressure introducing pipe 3 from the outside is kept constant, this slight voltage change is caused by the pressure change P1 inside the sensor, so that the vacuum leak rate can be estimated from the above-mentioned formula 1. As aforementioned,
If the vacuum leak is large and no discharge occurs, it is at least about 50 times the maximum allowable vacuum leak rate and 10
There is a pressure increase of 1000 Pa or more if left for a day (for example, if leaking at a speed 50 times faster, the pressure after 10 days becomes 1600 Pa (= 12 Torr)), and the voltage change with respect to this pressure increase is several mV. Therefore, the pressure change during that time, that is, the vacuum leakage rate can be roughly estimated by the mathematical formula 1 by measuring the voltage increase.

【0018】以上の結果から圧力センサーの実用的な真
空漏れ検査システムを考えれば、先ずセンサー製造日か
ら10日程度後に、外壁となる金属ケース6とすべての
電極2を短絡した端子間に600Vの直流電圧を印加
し、放電電流が流れれば、少なくとも0.77×10-5
Pa・cc/sec以上の速さで真空漏れが生じている
から不良品として取り除き、つぎに、たとえ放電が生じ
なくても4.6×10-4Pa・cc/sec以上の速さ
で真空漏れが生じている可能性があるので、圧力センサ
ー1の電極2に6Vの直流電圧を印加してその出力電圧
を記録しておき、さらに10日間程度放置後に出力電圧
を測定し、その電圧差が数mV以上であれば、これは最
大許容真空漏れ率の50倍以上の速さで漏れており不良
品ということになる。この場合、出力電圧は圧力センサ
ー1の内部と外部の圧力差(Px−P1)に比例するの
で、圧力導入パイプ3にはこの差(Px−P1)が常に
正となるように、即ちPxとしてその最大値4×104
Paを設定すれば良い。
From the above results, considering a practical vacuum leak inspection system for a pressure sensor, first, about 10 days after the sensor is manufactured, 600 V is applied between the terminals where the metal case 6 forming the outer wall and all the electrodes 2 are short-circuited. If a DC voltage is applied and a discharge current flows, at least 0.77 × 10 -5
Vacuum leakage occurs at a speed of Pa · cc / sec or more, so it is removed as a defective product, and then vacuum is generated at a speed of 4.6 × 10 −4 Pa · cc / sec or more even if no discharge occurs. Since there is a possibility that leakage has occurred, a direct current voltage of 6 V is applied to the electrode 2 of the pressure sensor 1 and the output voltage is recorded, and the output voltage is measured after leaving it for about 10 days. If the value is several mV or more, this is a defective product because it leaks at a speed 50 times or more the maximum allowable vacuum leak rate. In this case, the output voltage is proportional to the pressure difference (Px-P1) between the inside and the outside of the pressure sensor 1, so that the difference (Px-P1) is always positive in the pressure introducing pipe 3, that is, as Px. Its maximum value 4 × 10 4
It suffices to set Pa.

【0019】[0019]

【発明の効果】本発明に係る圧力センサーの良否判定方
法は以上説明してきたようなものなので、従来の放射能
利用による方法に代わって、真空漏れ及び電気回路的な
欠陥について放電と電気出力特性の両者から広範囲にわ
たって実用的に推定でき、しかも簡易かつ安全で、かつ
正確、無公害、経済的なものとなるという効果がある。
As described above, the method of judging the quality of the pressure sensor according to the present invention is the same as that described above. Therefore, instead of the conventional method using radioactivity, the discharge and electric output characteristics of vacuum leakage and electric circuit defects are eliminated. It is possible to estimate a wide range from both of the above, and it is simple and safe, accurate, pollution-free, and economical.

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

【図1】測定対象となる圧力センサーの構造を示す平面
断面図(A)及び側面部分断面図(B)である。
FIG. 1 is a plan sectional view (A) and a side partial sectional view (B) showing a structure of a pressure sensor to be measured.

【図2】図1の圧力センサーの測定系を示す概念図であ
る。
FIG. 2 is a conceptual diagram showing a measurement system of the pressure sensor of FIG.

【図3】図2の装置での放電電圧印加による放電結果を
示す図である。
FIG. 3 is a diagram showing a discharge result by applying a discharge voltage in the apparatus of FIG.

【図4】図2の装置での直流バイアス電圧印加による測
定結果を示す図である。
4 is a diagram showing a measurement result by applying a DC bias voltage in the apparatus of FIG.

【符号の説明】[Explanation of symbols]

1 圧力センサー 1a ベース 2 電極 3 圧力導入管 4 金属ダイアフラム 5 圧電素子 6 金属ケース 7 ロータリーポンプ 8 配管 9 ピラニー真空計 10 圧力調整弁 11 電源 12 電圧計 1 Pressure Sensor 1a Base 2 Electrode 3 Pressure Introducing Tube 4 Metal Diaphragm 5 Piezoelectric Element 6 Metal Case 7 Rotary Pump 8 Piping 9 Pirani Vacuum Gauge 10 Pressure Control Valve 11 Power Supply 12 Voltmeter

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 ケース内の真空度と圧力導入部に印加さ
れる圧力との差から生じる歪電圧によって圧力を測定す
る歪みゲージ式の圧力センサーについて真空漏れの良否
を判定する方法であって、センサー製造日から所定時間
経過後に、すべての電極を短絡した端子と上記ケースと
の間に所定値の直流高電圧を印加し、放電電流が流れれ
ば真空漏れが生じているものとして不良品と判断し、放
電が生じない場合には、上記電極に所定値の直流バイア
ス電圧を印加してその出力電圧を記録しておき、さらに
所定時間経過後に再び同じ値の直流バイアス電圧を印加
して出力電圧を測定し、測定した電圧差が所定値以上で
あれば真空漏れが生じているものとして不良品と判断す
ることを特徴とする圧力センサーの良否判定方法。
1. A method for determining the quality of a vacuum leak in a strain gauge type pressure sensor for measuring a pressure by a strain voltage generated from a difference between a degree of vacuum in a case and a pressure applied to a pressure introducing portion, After a lapse of a predetermined time from the sensor manufacturing date, a DC high voltage of a predetermined value was applied between the terminals with all the electrodes short-circuited and the case, and if discharge current flowed, it was determined that vacuum leakage had occurred and the product was defective. If it is judged that no discharge occurs, a DC bias voltage of a specified value is applied to the electrode and the output voltage is recorded, and then a DC bias voltage of the same value is applied again after a specified period of time to output. A method for determining the quality of a pressure sensor, which comprises measuring a voltage and determining that a vacuum leak has occurred if the measured voltage difference is equal to or more than a predetermined value, as a defective product.
JP35094895A 1995-12-25 1995-12-25 Method for deciding go/no-go of pressure sensor Pending JPH09178590A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP35094895A JPH09178590A (en) 1995-12-25 1995-12-25 Method for deciding go/no-go of pressure sensor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP35094895A JPH09178590A (en) 1995-12-25 1995-12-25 Method for deciding go/no-go of pressure sensor

Publications (1)

Publication Number Publication Date
JPH09178590A true JPH09178590A (en) 1997-07-11

Family

ID=18414004

Family Applications (1)

Application Number Title Priority Date Filing Date
JP35094895A Pending JPH09178590A (en) 1995-12-25 1995-12-25 Method for deciding go/no-go of pressure sensor

Country Status (1)

Country Link
JP (1) JPH09178590A (en)

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