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JPH0815079A - Instrument and method for measuring pressure leakage - Google Patents

Instrument and method for measuring pressure leakage

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Publication number
JPH0815079A
JPH0815079A JP15120494A JP15120494A JPH0815079A JP H0815079 A JPH0815079 A JP H0815079A JP 15120494 A JP15120494 A JP 15120494A JP 15120494 A JP15120494 A JP 15120494A JP H0815079 A JPH0815079 A JP H0815079A
Authority
JP
Japan
Prior art keywords
pressure
pipe
measured
differential pressure
measuring device
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.)
Granted
Application number
JP15120494A
Other languages
Japanese (ja)
Other versions
JP3186438B2 (en
Inventor
Hiroshi Horikawa
宏 堀川
Yukio Nakamura
幸雄 中村
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
Original Assignee
Toyota Motor Corp
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 filed Critical Toyota Motor Corp
Priority to JP15120494A priority Critical patent/JP3186438B2/en
Publication of JPH0815079A publication Critical patent/JPH0815079A/en
Application granted granted Critical
Publication of JP3186438B2 publication Critical patent/JP3186438B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Abstract

PURPOSE:To provide a pressure leakage measuring instrument which can measure pressure leakage with high accuracy by detecting a differential pressure with a simple constitution using no master for measurement and can be manufactured at a low cost. CONSTITUTION:At the time of measuring pressure leakage with a pressure leakage measuring instrument 2, all of opening/closing valves 20, 30, and 40 are opened and a pressurized gas is introduced into an object W to be measured through pipelines 10A-10E and into a pipeline 12B through pipelines 10A and 12A. After a prescribed period of time, the supply of the pressurized gas is discontinued by closing the valve 20 and, on the other hand, the internal pressures in the object W and pipelines 10C,..., 12B are made uniform by opening the valves 3 and 40 by prescribed balancing time more. After the balancing time, the valves 30 and 40 are closed and the differential pressure between a produced closed space 12B and the object W is measured by means of a differential pressure detector 8. When no gas leakage occurs from the object W, the measured differential pressure becomes zero and, when gas leakage exists, a differential pressure equal to the leaking-out amount of the gas is detected by means of the detector 8.

Description

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

【0001】[0001]

【産業上の利用分野】この発明は、被測定物内に加圧気
体源から加圧気体を導入して、被測定物内の圧力変化を
測定することによって、被測定物からの圧力洩れを測定
する圧力洩れ測定装置及び圧力洩れ測定方法に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention introduces a pressurized gas from a source of pressurized gas into an object to be measured and measures a pressure change in the object to be measured to prevent pressure leakage from the object to be measured. The present invention relates to a pressure leak measuring device and a pressure leak measuring method.

【0002】[0002]

【従来の技術】自動車エンジン用鋳造ブロック等の密閉
性を測定するために、被測定物の内部にエアコンプレッ
サ等の加圧気体源から圧縮空気等の加圧気体を導入し
て、被測定物からの圧力洩れを測定する方法が用いられ
る。この際、単に圧力センサによって被測定物からの圧
力洩れに伴う気圧の絶対値の変化を測定する方式では、
圧力センサの測定精度の制約があるため精度の良い圧力
洩れ測定ができない。そこで、高精度の圧力洩れ測定を
行うための装置として、被測定物とほぼ同一形状で気体
洩れのない測定用マスタ(以下、単に「マスタ」ともい
う。)を用意して、このマスタと被測定物とを差圧検出
器を介して接続し、差圧の変化を検出することによって
被測定物からの圧力洩れを測定するものが開発されてい
る。かかる差圧測定による圧力洩れ測定装置の具体例と
して、例えば、特開平4−221733号公報に記載さ
れた圧力洩れ測定装置の発明がある。この公報に記載さ
れた技術においては、被測定物とほぼ同一形状・同一容
積の測定用マスタと被測定物とが差圧検出器を介して接
続されている。そして、被測定物及びマスタ内に圧縮空
気が導入されて測定圧力に達した時点から差圧値の経時
変化を測定することによって、被測定物からの圧力洩れ
の測定が行われる。
2. Description of the Related Art In order to measure the hermeticity of a casting block for an automobile engine, a pressurized gas such as compressed air is introduced into a measured object from a pressurized gas source such as an air compressor to measure the measured object. A method is used to measure pressure leakage from the. At this time, in the method of simply measuring the change in the absolute value of the atmospheric pressure due to the pressure leak from the measured object by the pressure sensor
Due to the limitation of measurement accuracy of the pressure sensor, accurate pressure leak measurement cannot be performed. Therefore, as a device for performing highly accurate pressure leak measurement, a measurement master (hereinafter also simply referred to as “master”) having substantially the same shape as the object to be measured and having no gas leakage is prepared. There has been developed a device which is connected to a measurement object via a differential pressure detector and measures a pressure leak from the measurement object by detecting a change in the differential pressure. As a specific example of the pressure leak measuring device based on the differential pressure measurement, there is, for example, the invention of the pressure leak measuring device described in JP-A-4-221733. In the technique described in this publication, a measurement master having substantially the same shape and volume as the object to be measured and the object to be measured are connected via a differential pressure detector. Then, the pressure leakage from the measured object is measured by measuring the change over time of the differential pressure value from the time when the compressed air is introduced into the measured object and the master to reach the measured pressure.

【0003】[0003]

【発明が解決しようとする課題】しかしながら、かかる
マスタを使用する圧力洩れ測定装置においては、被測定
物とほぼ同一形状・同一容積で、しかも圧力洩れがない
マスタを作成しなければならない。一般に複雑な形状を
有する被測定物と同一形状のマスタを圧力洩れなく作成
するのは容易でなく、マスタ作成のための費用と工数が
大きくなる。さらに、多品種生産が行われている工程に
おいては被測定物が異なるごとに新たなマスタを準備し
なければならず、マスタの交換手段も必要となることか
ら圧力洩れ検査のためのコストが著しく高くなってしま
う。また、配管も複雑になることから装置の維持保全の
工数も大きくなり、マスタを交換するため測定時間も長
くかかる。これに対して、マスタの容量を変化させるこ
とによって一台で多種類の被測定物に対応できるように
した圧力洩れ測定装置も開発されているが、かかる可変
容量式マスタは極めて高価なものとなり、コスト高の問
題は解決されない。さらに、被測定物及びマスタ内に圧
縮空気が導入される際の温度変化等により圧力変動が生
ずるため、圧力が安定するまで待たなければならず、測
定時間の短縮に限界があるという問題点があった。
However, in a pressure leak measuring device using such a master, it is necessary to prepare a master having substantially the same shape and volume as the object to be measured and having no pressure leak. Generally, it is not easy to create a master having the same shape as a DUT having a complicated shape without pressure leakage, and the cost and man-hours for creating the master increase. Furthermore, in the process where a wide variety of products are produced, a new master must be prepared for each different object to be measured, and a master replacement means is also required, so the cost for pressure leak inspection is significantly high. It gets expensive. Further, since the piping becomes complicated, the number of man-hours for maintenance and maintenance of the device becomes large, and the measurement time is long because the master is replaced. On the other hand, a pressure leak measuring device has been developed that can handle multiple types of DUTs by changing the capacity of the master, but such a variable capacitance master becomes extremely expensive. , The problem of high cost is not solved. Furthermore, since pressure fluctuations occur due to temperature changes when compressed air is introduced into the DUT and the master, it is necessary to wait until the pressure stabilizes, and there is a problem that there is a limit to shortening the measurement time. there were.

【0004】そこで、本出願の請求項1から請求項5に
係る発明においては、マスタを使用することなく差圧検
出による圧力洩れ測定を行うことによって、低コストで
圧力洩れ測定を行うことができる圧力洩れ測定装置及び
圧力洩れ測定方法を提供することを目的とする。また、
請求項2に係る発明においては、マスタを使用しない圧
力洩れ測定装置を簡単な配管構成で実現することによっ
て、測定操作が簡単で装置の維持管理も容易な圧力洩れ
測定装置を提供することを目的とする。また、請求項3
に係る発明においては、マスタを使用しない圧力洩れ測
定装置において、被測定物内の加圧を速めるとともに配
管内の圧力をより均一にすることによって、短時間で精
密な圧力洩れ測定を行うことができる圧力洩れ測定装置
を提供することを目的とする。さらに、請求項4に係る
発明においては、被測定物内と配管内の圧力を等しくす
ることによって、気体の移動をなくして圧力を安定さ
せ、より短時間でより精密な圧力洩れ測定を行える圧力
洩れ測定装置を提供することを目的とする。また、請求
項5に係る発明においては、圧力が安定する過程におい
て測定結果を求めることによって、測定時間を著しく短
縮できる圧力洩れ測定方法を提供することを目的とす
る。
Therefore, in the inventions according to claims 1 to 5 of the present application, pressure leak measurement can be performed at low cost by performing pressure leak measurement by differential pressure detection without using a master. An object is to provide a pressure leak measuring device and a pressure leak measuring method. Also,
In the invention according to claim 2, an object of the present invention is to provide a pressure leak measuring device that does not use a master and has a simple piping configuration, so that the measuring operation is easy and the device is easy to maintain. And Claim 3
According to the invention of claim 1, in a pressure leak measuring device that does not use a master, it is possible to perform accurate pressure leak measurement in a short time by speeding up the pressurization inside the object to be measured and making the pressure inside the pipe more uniform. An object of the present invention is to provide a pressure leakage measuring device that can be used. Further, in the invention according to claim 4, by making the pressure in the object to be measured equal to the pressure in the pipe, the pressure is stabilized by eliminating the movement of gas, and a more accurate pressure leak measurement can be performed in a shorter time. It is an object of the present invention to provide a leak measuring device. Further, it is an object of the invention according to claim 5 to provide a pressure leakage measuring method capable of remarkably shortening the measuring time by obtaining the measuring result in the process of stabilizing the pressure.

【0005】[0005]

【課題を解決するための手段】そこで、上記の課題を解
決するために、請求項1に係る発明においては、加圧気
体が導入された被測定物と独立した密閉空間との差圧を
検出することによって前記被測定物からの圧力洩れを測
定する圧力洩れ測定装置であって、前記独立した密閉空
間を前記圧力洩れ測定装置の配管の一部を閉鎖すること
によって形成する圧力洩れ測定装置を創出した。ここで
「加圧気体」とは、圧縮空気を始めとして圧縮窒素ガ
ス,圧縮酸素ガス,圧縮アルゴンガス等の種々の気体を
含むものである。
Therefore, in order to solve the above-mentioned problems, in the invention according to claim 1, the differential pressure between the object to be measured into which the pressurized gas is introduced and the closed space which is independent is detected. A pressure leak measuring device for measuring pressure leak from the object to be measured, wherein the independent sealed space is formed by closing a part of the piping of the pressure leak measuring device. Created. Here, the "pressurized gas" includes various gases such as compressed air, compressed nitrogen gas, compressed oxygen gas, compressed argon gas and the like.

【0006】また請求項2に係る発明においては、請求
項1に記載された圧力洩れ測定装置であって、前記被測
定物に加圧気体を導入するための加圧気体源を前記被測
定物と接続する第一の配管と、その両端が各々前記加圧
気体源に近い側の第一接続部と前記被測定物に近い側の
第二接続部において前記第一の配管に接続された第二の
配管と、該第二の配管に設けられた差圧検出器と、該差
圧検出器と前記第一接続部との間において前記第二の配
管に設けられた第一の開閉弁と、前記加圧気体源と前記
第二接続部との間において前記第一の配管に設けられた
第二の開閉弁とを有する圧力洩れ測定装置を創出した。
ここで「加圧気体源」とは、圧縮空気を供給するエアコ
ンプレッサや、窒素ガス,アルゴンガス等の種々のガス
を高圧で封入したガスボンベ等を含むものである。
According to a second aspect of the present invention, in the pressure leak measuring device according to the first aspect, the pressurized gas source for introducing the pressurized gas into the object to be measured is the object to be measured. A first pipe connected to the first pipe, and both ends thereof are connected to the first pipe at a first connection part on the side closer to the pressurized gas source and a second connection part on the side closer to the DUT. A second pipe, a differential pressure detector provided on the second pipe, and a first opening / closing valve provided on the second pipe between the differential pressure detector and the first connecting portion. A pressure leak measuring device having a second on-off valve provided in the first pipe between the pressurized gas source and the second connecting portion is created.
Here, the "pressurized gas source" includes an air compressor that supplies compressed air, a gas cylinder in which various gases such as nitrogen gas and argon gas are sealed at high pressure, and the like.

【0007】さらに、請求項3に係る発明においては、
請求項2に記載された圧力洩れ測定装置であって、その
一端が前記第一の開閉弁と前記差圧検出器との間におい
て前記第二の配管に接続され、他端が前記被測定物に接
続された第三の配管と、該第三の配管に設けられた第三
の開閉弁とを有する圧力洩れ測定装置を創出した。
Further, in the invention according to claim 3,
The pressure leak measuring device according to claim 2, wherein one end is connected to the second pipe between the first opening / closing valve and the differential pressure detector, and the other end is the object to be measured. A pressure leak measuring device having a third pipe connected to the above and a third opening / closing valve provided in the third pipe was created.

【0008】また、請求項4に係る発明においては、加
圧気体が導入された被測定物と独立した密閉空間との差
圧を検出することによって前記被測定物からの圧力洩れ
を測定する圧力洩れ測定装置であって、前記被測定物に
加圧気体を導入するための加圧気体源を前記被測定物と
接続する一次側配管と、該一次側配管に設けられた一次
側開閉弁と、前記被測定物に二次側配管を介して接続さ
れた閉ループ状の配管と、前記閉ループ状配管に設けら
れた差圧検出器及び閉ループ開閉弁とを有する圧力洩れ
測定装置を創出した。
Further, in the invention according to claim 4, a pressure for measuring pressure leakage from the object to be measured is detected by detecting a differential pressure between the object to be measured into which the pressurized gas is introduced and an independent closed space. A leak measuring apparatus, wherein a primary side pipe connecting a pressurized gas source for introducing a pressurized gas to the measurement object and the measurement object, and a primary side opening / closing valve provided in the primary side pipe A pressure leak measuring device having a closed loop pipe connected to the object to be measured via a secondary pipe, and a differential pressure detector and a closed loop on-off valve provided in the closed loop pipe is created.

【0009】さらに、請求項5に係る発明においては、
被測定物に加圧気体を導入して、独立した密閉空間と前
記被測定物との差圧を検出することによって前記被測定
物からの圧力洩れを測定する圧力洩れ測定方法であっ
て、前記差圧の単位時間当たりの変化量から所定時間経
過後の前記差圧の大きさを予測することによって前記被
測定物からの圧力洩れを測定する圧力洩れ測定方法を創
出した。
Further, in the invention according to claim 5,
Introducing a pressurized gas to the object to be measured, a pressure leak measuring method for measuring pressure leakage from the object to be measured by detecting a differential pressure between an independent closed space and the object to be measured, A pressure leak measuring method for measuring the pressure leak from the object to be measured by predicting the magnitude of the differential pressure after a lapse of a predetermined time from the variation amount of the differential pressure per unit time is created.

【0010】[0010]

【作用】さて、請求項1の発明に係る圧力洩れ測定装置
は、加圧気体が導入された被測定物と独立した密閉空間
との差圧を検出することによって、被測定物からの圧力
洩れを測定する装置である。ここで、独立した密閉空間
は、圧力洩れ測定装置の配管の一部を閉鎖することによ
って形成される。従って、従来技術における測定用マス
タと異なり高度な密閉性が確保され、圧力洩れのない密
閉空間が容易に実現される。これによって、多種多様な
被測定物についてこの密閉空間との差圧を検出して高精
度の圧力洩れ測定を実施することができ、しかもマスタ
を使用せず配管の一部を利用しているため、極めて低コ
ストの圧力洩れ測定装置となる。このようにして、マス
タを使用することなく差圧検出による圧力洩れ測定を行
うことによって、低コストで圧力洩れ測定を行うことが
できる圧力洩れ測定装置となる。
In the pressure leak measuring apparatus according to the first aspect of the present invention, the pressure leak from the measured object is detected by detecting the differential pressure between the measured object into which the pressurized gas is introduced and the closed space independent from the measured object. Is a device for measuring. Here, the independent closed space is formed by closing a part of the piping of the pressure leak measuring device. Therefore, unlike the measurement master in the prior art, a high degree of airtightness is ensured and a pressure-tight sealed space is easily realized. This makes it possible to detect the pressure difference between this and the enclosed space for a wide variety of objects to be measured and to perform highly accurate pressure leak measurement, and because a part of piping is used without using a master. It becomes an extremely low cost pressure leak measuring device. In this way, the pressure leak measurement apparatus can perform the pressure leak measurement at low cost by performing the pressure leak measurement by detecting the differential pressure without using the master.

【0011】また、請求項2の発明に係る圧力洩れ測定
装置においては、加圧気体源と被測定物とを接続する第
一の配管に対して第二の配管の両端が接続されており、
加圧気体のバイパス経路が設けられている。そして、第
二の配管には差圧検出器が設けられており、差圧検出器
と第一接続部との間には第一の開閉弁が設けられてい
る。さらに、第一の配管には、加圧気体源と第二接続部
との間のいずれかの位置において、第二の開閉弁が設け
られている。従って、第一の開閉弁が閉じられることに
よって、第二の配管のうち第一の開閉弁と差圧検出器に
挟まれた部分によって、独立した密閉空間が形成され
る。一方、被測定物は、第一の配管のうち被測定物から
第二接続部までの部分と、第二の配管のうち第二接続部
から差圧検出器までの部分によって、差圧検出器に接続
されている。かかる構成によって、加圧気体源から第一
の配管を通じて被測定物に加圧気体が導入された後に第
一の開閉弁及び第二の開閉弁が閉じられることによっ
て、独立した密閉空間と被測定物との差圧が差圧検出器
によって検出される。従って、密閉度が高度に保たれた
密閉空間と被測定物との差圧を検出することができる。
しかも、必要最小限の配管構成によって差圧検出による
圧力洩れを測定しているため、極めて低コストの圧力洩
れ測定装置となる。このようにして、マスタを使用しな
い圧力洩れ測定装置を簡単な配管構成で実現することに
よって、測定操作が簡単で装置の維持管理も容易な圧力
洩れ測定装置となる。
Further, in the pressure leak measuring device according to the invention of claim 2, both ends of the second pipe are connected to the first pipe connecting the pressurized gas source and the object to be measured,
A bypass path for pressurized gas is provided. A differential pressure detector is provided on the second pipe, and a first opening / closing valve is provided between the differential pressure detector and the first connecting portion. Further, the first pipe is provided with a second opening / closing valve at any position between the pressurized gas source and the second connection portion. Therefore, when the first opening / closing valve is closed, an independent closed space is formed by the portion of the second pipe sandwiched between the first opening / closing valve and the differential pressure detector. On the other hand, the object to be measured is a differential pressure detector by a part of the first pipe from the object to be measured to the second connection part and a part of the second pipe from the second connection part to the differential pressure detector. It is connected to the. With such a configuration, after the pressurized gas is introduced into the DUT from the pressurized gas source through the first pipe, the first opening / closing valve and the second opening / closing valve are closed, thereby providing an independent closed space and an object to be measured. The differential pressure with the object is detected by the differential pressure detector. Therefore, it is possible to detect the differential pressure between the object to be measured and the hermetically sealed space with a high degree of hermeticity.
Moreover, since the pressure leak is detected by the differential pressure detection with the minimum necessary piping configuration, the pressure leak measuring device can be provided at an extremely low cost. In this way, the pressure leak measuring device that does not use the master is realized with a simple piping configuration, so that the pressure leak measuring device has a simple measurement operation and easy maintenance of the device.

【0012】また、請求項3の発明に係る圧力洩れ測定
装置は、請求項2の発明に係る圧力洩れ測定装置に対し
て、その一端が第一の開閉弁と差圧検出器との間におい
て第二の配管に接続され他端が被測定物に接続された第
三の配管と、この第三の配管に設けられた第三の開閉弁
とを追加した構成を有している。従って、加圧気体源か
ら第一の配管及び第三の配管の二つの経路によって被測
定物に加圧気体を導入できるため、被測定物内の圧力を
速く測定圧力まで高めることができる。さらに、この第
三の配管によって第二の配管のうち独立した密閉空間と
なる部分と被測定物とを連通させることができるため、
両者の圧力差を小さくでき、配管内の圧力がより速く安
定することから測定時間を短縮できる。そして、差圧測
定時には第三の開閉弁を閉じることによって被測定物と
の連通が遮断される。このようにして、被測定物内の加
圧を速めるとともに配管内の圧力をより均一にすること
によって、短時間で精密な圧力洩れ測定を行うことがで
きる圧力洩れ測定装置となる。
Further, a pressure leak measuring device according to a third aspect of the present invention is different from the pressure leak measuring device according to the second aspect in that one end of the pressure leak measuring device is between the first opening / closing valve and the differential pressure detector. It has a configuration in which a third pipe connected to the second pipe and the other end of which is connected to the object to be measured, and a third opening / closing valve provided in the third pipe are added. Therefore, since the pressurized gas can be introduced from the pressurized gas source into the object to be measured through the two paths of the first pipe and the third pipe, the pressure inside the object to be measured can be quickly increased to the measurement pressure. Furthermore, since the third pipe can connect the part to be the closed space independent of the second pipe and the DUT,
The pressure difference between the two can be made small, and the pressure in the pipe stabilizes faster, so the measurement time can be shortened. When measuring the differential pressure, the third on-off valve is closed to cut off communication with the object to be measured. In this way, the pressure leak measuring apparatus can perform precise pressure leak measurement in a short time by accelerating the pressurization inside the object to be measured and making the pressure inside the pipe more uniform.

【0013】さらに、請求項4の発明に係る圧力洩れ測
定装置においては、一次側開閉弁を備えた一次側配管に
よって加圧気体源に被測定物が接続され、この被測定物
に二次側配管を介して閉ループ状の配管が接続されてい
る。そして、この閉ループ状配管のうち、差圧検出器及
び閉ループ開閉弁とに挟まれた部分によって、差圧測定
のための密閉空間が形成される。一方、被測定物は閉ル
ープ状配管のうち密閉空間を形成する部分を除く部分に
よって、差圧検出器に接続されている。かかる構成によ
って、加圧気体源から一次側配管を通じて被測定物に加
圧気体が導入された後に一次側開閉弁及び閉ループ開閉
弁が閉じられて、独立した密閉空間と被測定物との差圧
が差圧検出器によって検出される。ここで、加圧気体は
被測定物を通って閉ループ状配管に導入されるため、密
閉空間と被測定物の圧力が等しくなる。従って、気体の
移動が起こらず圧力が安定することから、非常に小さな
差圧の発生をも検出することができ、高精度の圧力洩れ
測定が可能になる。さらに、容積の大きい被測定物が加
圧気体源に近接して設けられていることと相俟って、短
時間で圧力が安定して測定が可能になる。このようにし
て、被測定物内と配管内の圧力を等しくすることによっ
て、気体の移動をなくして圧力を安定させ、より短時間
でより精密な圧力洩れ測定を行うことができる圧力洩れ
測定装置となる。
Further, in the pressure leak measuring apparatus according to the invention of claim 4, the object to be measured is connected to the pressurized gas source by the primary side pipe provided with the primary side opening / closing valve, and the object to be measured is connected to the secondary side. A closed loop pipe is connected via the pipe. Then, of the closed loop pipe, a portion sandwiched between the differential pressure detector and the closed loop on-off valve forms a closed space for measuring the differential pressure. On the other hand, the object to be measured is connected to the differential pressure detector by the part of the closed loop pipe except the part forming the closed space. With such a configuration, after the pressurized gas is introduced from the pressurized gas source to the DUT through the primary side pipe, the primary side opening / closing valve and the closed loop opening / closing valve are closed, and the differential pressure between the independent sealed space and the DUT is measured. Is detected by the differential pressure detector. Here, since the pressurized gas is introduced into the closed loop pipe through the object to be measured, the pressure in the closed space becomes equal to that of the object to be measured. Therefore, since the gas does not move and the pressure is stable, it is possible to detect the occurrence of a very small differential pressure, and it is possible to measure the pressure leak with high accuracy. Further, in combination with the fact that the object to be measured having a large volume is provided close to the pressurized gas source, the pressure can be stably measured in a short time. In this way, by making the pressure inside the object to be measured equal to the pressure inside the pipe, the pressure is stabilized by eliminating the movement of gas, and a more accurate pressure leak measurement can be performed in a shorter time. Becomes

【0014】さらに、請求項5の発明に係る圧力洩れ測
定方法においては、独立した密閉空間と被測定物との差
圧を検出するに際して、差圧の単位時間当たりの変化量
から所定時間経過後の差圧の大きさを予測する方式を採
用している。従って、圧力が安定する過程における差圧
の変化率から所定時間経過後の差圧を予測して圧力洩れ
の大きさを求めることができるため、圧力が安定するま
で待つ必要がなく、極めて短時間に圧力洩れ測定を行う
ことができる。このようにして、圧力が安定する過程に
おいて測定結果を求めることによって、測定時間を著し
く短縮できる圧力洩れ測定方法となる。
Furthermore, in the pressure leak measuring method according to the fifth aspect of the present invention, when the differential pressure between the independent closed space and the object to be measured is detected, after a lapse of a predetermined time from the change amount of the differential pressure per unit time. The method of predicting the magnitude of the differential pressure is adopted. Therefore, it is possible to predict the pressure difference after a lapse of a predetermined time from the rate of change of the pressure difference in the process of stabilizing the pressure to determine the magnitude of pressure leakage, so that it is not necessary to wait until the pressure stabilizes, and it is possible to obtain an extremely short time. It is possible to perform pressure leak measurement. In this way, by obtaining the measurement result in the process of stabilizing the pressure, the pressure leakage measuring method can be shortened remarkably.

【0015】[0015]

【実施例】【Example】

実施例1 次に、本発明を具現化した実施例1について図1及び図
2を参照して説明する。まず、本実施例の圧力洩れ測定
装置の基本的な構成及び操作について、図1を参照して
説明する。図1(A)は本実施例の圧力洩れ測定装置2
の基本的構成を示すブロック図であり、図1(B)は開
閉弁の開閉を示すチャート図である。図1(A)に示さ
れる圧力洩れ測定装置2は、加圧気体源4と、加圧気体
源4を被測定物W及び差圧検出器8と接続する配管系及
び配管系に設けられた開閉弁20,30,40を中心と
して構成されている。加圧気体源4は配管10Aによっ
て開閉弁20に接続され、開閉弁20の他端は配管10
Bに接続されている。配管10Bは分岐部14Aにおい
て配管10Cと配管12Aに分岐している。配管10C
は開閉弁30に接続され、開閉弁30の他端は配管10
Dに接続されている。配管10Dは、分岐部14Bにお
いて配管10Eと配管12Cに分岐しており、配管10
Eは被測定物Wに接続され、配管12Cは差圧検出器8
の測定部の片側に接続されている。一方、配管12Aは
開閉弁40に接続され、開閉弁40の他端は配管12B
に接続されている。配管12Bは、差圧検出器8の測定
部のもう一方の側に接続されている。配管12Bにはエ
アチャンバACが接続されている。
First Embodiment Next, a first embodiment embodying the present invention will be described with reference to FIGS. 1 and 2. First, the basic configuration and operation of the pressure leakage measuring device of this embodiment will be described with reference to FIG. FIG. 1A shows a pressure leak measuring device 2 of this embodiment.
FIG. 1B is a block diagram showing the basic configuration of FIG. 1B, and FIG. 1B is a chart showing the opening and closing of the on-off valve. The pressure leak measuring device 2 shown in FIG. 1 (A) is provided in the pressurized gas source 4, the piping system connecting the pressurized gas source 4 to the object W to be measured and the differential pressure detector 8, and the piping system. The on-off valves 20, 30, 40 are mainly configured. The pressurized gas source 4 is connected to the opening / closing valve 20 by a pipe 10A, and the other end of the opening / closing valve 20 is connected to the pipe 10
Connected to B. The pipe 10B branches into a pipe 10C and a pipe 12A at a branch portion 14A. Piping 10C
Is connected to the on-off valve 30, and the other end of the on-off valve 30 is connected to the pipe 10
D. The pipe 10D is branched into a pipe 10E and a pipe 12C at a branch portion 14B.
E is connected to the object to be measured W, and the pipe 12C is connected to the differential pressure detector 8
It is connected to one side of the measurement part of. On the other hand, the pipe 12A is connected to the open / close valve 40, and the other end of the open / close valve 40 is connected to the pipe 12B.
It is connected to the. The pipe 12B is connected to the other side of the measuring unit of the differential pressure detector 8. An air chamber AC is connected to the pipe 12B.

【0016】かかる構成を有する圧力洩れ測定装置2に
おいて、加圧気体が導入された被測定物Wと独立した密
閉空間とされた配管12Bとの差圧を差圧検出器8で測
定することによって、被測定物Wの圧力洩れが測定され
る。すなわち、図1(B)に示されるように、まず開閉
弁20,30,40が全て開けられて、加圧気体源4か
ら被測定物W及び配管12B内に加圧気体が導入され
る。続いて、一定時間だけ開閉弁20のみが閉じられ
て、被測定物W内の気圧と配管12B内の気圧との平衡
が図られる。その後、開閉弁30,40が閉じられて、
開閉弁40と差圧検出器8で挟まれた配管12Bとエア
チャンバACが独立した密閉空間とされる。この密閉空
間12BとエアチャンバAC内の気圧と被測定物W内の
気圧との差圧が、差圧検出器8において測定される。こ
こで、開閉弁40と差圧検出器8で挟まれた配管12B
の部分とエアチャンバACは、洩れのない独立した密閉
空間と見做せる。また、平衡操作によって配管12B内
の気圧と被測定物W内の気圧は一旦平衡に達しているこ
とから、被測定物Wからの気体洩れがない場合には、差
圧検出器8で測定される差圧はゼロとなる。これに対し
て、被測定物Wからの気体洩れがあれば、差圧検出器8
によって気体洩れ分だけの差圧が検出されることにな
る。なおこの実施例では、エアチャンバACが設けられ
ているために、差圧の検出感度が向上している。
In the pressure leak measuring device 2 having such a structure, the differential pressure between the measured object W into which the pressurized gas is introduced and the pipe 12B, which is an independent closed space, is measured by the differential pressure detector 8. The pressure leakage of the object to be measured W is measured. That is, as shown in FIG. 1 (B), first, all the on-off valves 20, 30, 40 are opened, and pressurized gas is introduced from the pressurized gas source 4 into the measured object W and the pipe 12B. Subsequently, only the on-off valve 20 is closed for a certain period of time to balance the atmospheric pressure inside the object to be measured W and the atmospheric pressure inside the pipe 12B. After that, the on-off valves 30 and 40 are closed,
The pipe 12 </ b> B sandwiched between the on-off valve 40 and the differential pressure detector 8 and the air chamber AC form an independent closed space. The differential pressure between the atmospheric pressure inside the closed space 12B and the air chamber AC and the atmospheric pressure inside the object to be measured W is measured by the differential pressure detector 8. Here, the pipe 12B sandwiched between the on-off valve 40 and the differential pressure detector 8
Can be regarded as an independent closed space without leakage. Further, since the atmospheric pressure in the pipe 12B and the atmospheric pressure in the object to be measured W have once reached equilibrium due to the equilibrium operation, if there is no gas leakage from the object to be measured W, the pressure difference is measured by the differential pressure detector 8. The differential pressure is zero. On the other hand, if gas leaks from the object to be measured W, the differential pressure detector 8
Therefore, the differential pressure corresponding to the gas leakage is detected. In this embodiment, since the air chamber AC is provided, the differential pressure detection sensitivity is improved.

【0017】圧力洩れ測定装置2のより具体的な構成と
測定の手順について、図2を参照して説明する。図2
(A)は圧力洩れ測定装置2の具体的構成を示す配管図
であり、図2(B)は圧力洩れ測定の手順を示すチャー
ト図である。図2(A)に示されるように、圧力洩れ測
定装置2は加圧気体源としてエアコンプレッサ4を用い
ている。エアコンプレッサ4は、圧縮空気中の粉塵等を
除去するエアフィルタ6を介して、配管10Aによって
電磁方向弁20に接続されている。電磁方向弁20の対
向するポートには、配管10Bが接続されている。この
電磁方向弁20は三つの弁室24A,24B,24Cを
有しており、電磁ソレノイド22の非作動時には、スプ
リング26の付勢力によって、弁室24Cが配管10A
及び配管10Bに接続される。すなわち、図2(A)に
示される状態となる。このとき、配管10Aは閉状態の
ポートに接続され、一方配管10Bは排気消音器28に
通ずるポートに接続された状態となる。これによって、
配管10B以降の配管及び被測定物W,差圧検出器8内
に残留していた圧縮空気が、排気消音器28から大気中
に放出される。
A more specific structure of the pressure leak measuring device 2 and a measuring procedure will be described with reference to FIG. Figure 2
(A) is a piping diagram showing a specific configuration of the pressure leak measuring device 2, and FIG. 2 (B) is a chart diagram showing a procedure for pressure leak measuring. As shown in FIG. 2A, the pressure leak measuring device 2 uses an air compressor 4 as a pressurized gas source. The air compressor 4 is connected to the electromagnetic directional valve 20 by a pipe 10A via an air filter 6 that removes dust and the like in the compressed air. A pipe 10B is connected to the opposing port of the electromagnetic directional valve 20. The electromagnetic directional valve 20 has three valve chambers 24A, 24B and 24C, and when the electromagnetic solenoid 22 is inactive, the valve chamber 24C is connected to the pipe 10A by the urging force of the spring 26.
And the pipe 10B. That is, the state shown in FIG. At this time, the pipe 10A is connected to the closed port, while the pipe 10B is connected to the port communicating with the exhaust silencer 28. by this,
The compressed air remaining in the pipe 10B and subsequent pipes, the object to be measured W, and the differential pressure detector 8 is discharged from the exhaust silencer 28 into the atmosphere.

【0018】一方、図示しない制御ユニットからの制御
信号によって電磁ソレノイド22が励磁されると、弁室
24A,24B,24Cがスプリング26の付勢力に抗
して移動する。励磁力が低い状態に制御された場合に
は、中央の弁室24Bが配管10Aに接続される。これ
によって、配管10A,配管10Bはいずれも閉状態の
ポートに接続され、配管10Bとエアコンプレッサ4及
び排気消音器28の間は遮断されて、配管10B以降の
配管系が密閉された状態となる。さらに、励磁力が高い
状態に制御された場合には、弁室24Aが配管10Aに
接続される。これによって、配管10Aと配管10Bが
接続された状態となり、エアコンプレッサ4から圧縮空
気が配管系に供給される。
On the other hand, when the electromagnetic solenoid 22 is excited by a control signal from a control unit (not shown), the valve chambers 24A, 24B and 24C move against the biasing force of the spring 26. When the excitation force is controlled to be low, the central valve chamber 24B is connected to the pipe 10A. As a result, both the pipe 10A and the pipe 10B are connected to the closed ports, the pipe 10B and the air compressor 4 and the exhaust silencer 28 are shut off, and the pipe system after the pipe 10B is sealed. . Further, when the excitation force is controlled to be high, the valve chamber 24A is connected to the pipe 10A. As a result, the pipe 10A and the pipe 10B are connected, and compressed air is supplied from the air compressor 4 to the pipe system.

【0019】配管10Bは分岐部14Aで配管10Cと
配管12Aに分岐し、配管10Cは電磁開閉弁30に接
続され、配管12Aは電磁開閉弁40に接続されてい
る。電磁開閉弁30は二つの弁室34A,34Bを有し
ており、電磁ソレノイド32の非作動時においては、ス
プリング36の反発力によって、閉状態の弁室34Bが
配管10Cに接続されている。一方、電磁ソレノイド3
2が作動すると、弁室34A,34Bがスプリング36
の反発力に抗して移動して、開状態の弁室34Aが配管
10Cに接続される。電磁開閉弁40も、電磁開閉弁3
0と同様の構造を有している。電磁開閉弁30の他端は
配管10Dに接続されており、配管10Dは分岐部14
Bにおいて配管10Eと配管12Cに分岐している。配
管10Eは被測定物Wに接続され、配管12Cは差圧セ
ンサ8に接続されている。さらに、分岐部14Bには圧
力センサ16Aも接続されている。一方、電磁開閉弁4
0の他端は配管12Bに接続されており、配管12Bは
差圧センサ8に接続されている。また、配管12Bの途
中には、圧力センサ16BとエアチャンバACが接続さ
れている。
The pipe 10B is branched into a pipe 10C and a pipe 12A at a branch portion 14A, the pipe 10C is connected to the electromagnetic opening / closing valve 30, and the pipe 12A is connected to the electromagnetic opening / closing valve 40. The electromagnetic opening / closing valve 30 has two valve chambers 34A and 34B, and when the electromagnetic solenoid 32 is not operated, the valve chamber 34B in the closed state is connected to the pipe 10C by the repulsive force of the spring 36. On the other hand, the electromagnetic solenoid 3
2 is activated, the valve chambers 34A and 34B move to the spring 36.
The valve chamber 34A in the open state is connected to the pipe 10C by moving against the repulsive force of. The solenoid on-off valve 40 is also the solenoid on-off valve 3
It has the same structure as 0. The other end of the electromagnetic opening / closing valve 30 is connected to the pipe 10D, and the pipe 10D is connected to the branch portion 14
At B, a pipe 10E and a pipe 12C are branched. The pipe 10E is connected to the measured object W, and the pipe 12C is connected to the differential pressure sensor 8. Further, a pressure sensor 16A is also connected to the branch portion 14B. On the other hand, the solenoid valve 4
The other end of 0 is connected to the pipe 12B, and the pipe 12B is connected to the differential pressure sensor 8. A pressure sensor 16B and an air chamber AC are connected in the middle of the pipe 12B.

【0020】かかる構成を有する圧力洩れ測定装置2に
よる圧力洩れ測定の各段階について、図2(A)及び図
2(B)を参照しつつ説明する。ここで、Pm1は圧力セ
ンサ16Bによって測定される圧力を示し、圧力PX1
圧力センサ16Aによって測定される圧力を、またPW1
は被測定物W内の圧力を示す。図2(B)に示されるよ
うに、まず加圧操作として、電磁弁20,30,40が
全て開状態(弁室24A,34A,44Aが接続された
状態)とされる。これによって、エアコンプレッサ4か
ら配管10A,10B,10C,10D及び10Eを通
じて、被測定物W内に圧縮空気が導入され、また配管1
2C内にも圧縮空気が導入される。同時に、配管10
A,10B,12Aを通じて,配管12Bとエアチャン
バAC内にも圧縮空気が導入される。かかる加圧操作が
所定時間T1だけ行われた後、電磁方向弁20が切替え
られてエアコンプレッサ4からの圧縮空気の供給が遮断
される。この段階では電磁開閉弁30,40は開けられ
ているために、配管12A,12B及び配管10C,1
0D,10E,被測定物Wからなる密閉空間が一時的に
形成される。かかる状態が所定時間T2だけ維持される
ことによって、被測定物W及び配管10C,…,12B
内の圧力が均等化され、圧力Pm1とPX1とが平衡に達す
る。
Each stage of pressure leak measurement by the pressure leak measuring device 2 having such a configuration will be described with reference to FIGS. 2 (A) and 2 (B). Here, P m1 indicates the pressure measured by the pressure sensor 16B, pressure P X1 indicates the pressure measured by the pressure sensor 16A, and P W1
Indicates the pressure inside the object to be measured W. As shown in FIG. 2B, as a pressurizing operation, all of the solenoid valves 20, 30, 40 are first opened (the valve chambers 24A, 34A, 44A are connected). As a result, compressed air is introduced into the object to be measured W from the air compressor 4 through the pipes 10A, 10B, 10C, 10D and 10E, and the pipe 1
Compressed air is also introduced into 2C. At the same time, pipe 10
Compressed air is also introduced into the pipe 12B and the air chamber AC through A, 10B, and 12A. After the pressurizing operation is performed for a predetermined time T1, the electromagnetic directional valve 20 is switched to shut off the supply of compressed air from the air compressor 4. At this stage, since the solenoid on-off valves 30 and 40 are opened, the pipes 12A and 12B and the pipes 10C and 1
A sealed space including 0D, 10E and the object to be measured W is temporarily formed. By maintaining such a state for a predetermined time T2, the DUT W and the pipes 10C, ..., 12B are
The pressure inside is equalized and the pressures P m1 and P X1 reach equilibrium.

【0021】なお、この平衡段階において圧力センサ1
6A,16Bによる測定圧力PX1,Pm1が降下する場合
には、被測定物Wあるいは配管系に大きな洩れがあると
判断して、測定を中止する。かかる平衡操作が所定時間
T2だけ行われた後に、電磁開閉弁30,40が閉じら
れて配管12BとエアチャンバACが独立した密閉空間
とされ、差圧センサ8によって被測定物Wと配管12B
の差圧が測定される。この検出段階において、被測定物
Wからの空気洩れがある場合には、圧力Pm1は変化しな
いのに対して圧力PX1は低下するため、両者の差圧が検
出される。これに対して、被測定物Wからの空気洩れが
ない場合には、圧力PX1は圧力Pm1と同じ値に保たれる
ため、差圧センサ8で測定される差圧はゼロとなる。従
って、差圧センサ8からの出力信号を図示しない制御ユ
ニットで解析することによって、被測定物Wからの空気
洩れの有無とその大きさを測定できる。かかる検出操作
が所定時間T3だけ行われて、圧力洩れ測定装置2によ
る圧力洩れ測定は終了する。
At this equilibrium stage, the pressure sensor 1
When the measured pressures P X1 and P m1 by 6A and 16B drop, it is judged that there is a large leak in the object to be measured W or the piping system, and the measurement is stopped. After the equilibrium operation is performed for a predetermined time T2, the electromagnetic on-off valves 30 and 40 are closed to form the pipe 12B and the air chamber AC as an independent closed space, and the differential pressure sensor 8 and the measured object W and the pipe 12B are used.
The differential pressure of is measured. At this detection stage, when there is air leakage from the object to be measured W, the pressure P m1 does not change but the pressure P X1 decreases, so that the pressure difference between the two is detected. On the other hand, when there is no air leakage from the object to be measured W, the pressure P X1 is maintained at the same value as the pressure P m1 , so that the differential pressure measured by the differential pressure sensor 8 becomes zero. Therefore, by analyzing the output signal from the differential pressure sensor 8 by a control unit (not shown), the presence or absence of air leakage from the object to be measured W and its magnitude can be measured. The detection operation is performed for the predetermined time T3, and the pressure leak measurement by the pressure leak measurement device 2 is completed.

【0022】以上のようにして、本実施例の圧力洩れ測
定装置2においては、簡単な構成で精度良く、被測定物
Wからの空気洩れの有無とその大きさを測定することが
できる。なお、測定終了後には、各電磁弁20,30,
40の電磁ソレノイド22,32,42の作動が解除さ
れることによって弁室24C,34B,44Bが各配管
に接続され、被測定物W及び配管系内の圧縮空気が排気
消音器28から排出される。このように、本実施例の圧
力洩れ測定装置2においては従来技術のようなマスタを
使用することなく、装置を構成する配管10A,10
B,12A,12Bの一部12Bを電磁開閉弁40で閉
鎖して形成される独立した密閉空間との差圧を検出する
ことによって、圧力洩れ測定を行っている。従って、圧
力洩れ測定装置2の構成を組み替えることなく、多種類
の被測定物Wについて差圧測定ができ、低コストで圧力
洩れ測定を行える圧力洩れ測定装置となる。
As described above, in the pressure leakage measuring device 2 of the present embodiment, the presence or absence of air leakage from the object W to be measured and its magnitude can be measured with a simple structure and high accuracy. After the measurement, each solenoid valve 20, 30,
By releasing the operation of the electromagnetic solenoids 22, 32, 42 of 40, the valve chambers 24C, 34B, 44B are connected to the pipes, and the measured object W and the compressed air in the pipe system are discharged from the exhaust silencer 28. It As described above, in the pressure leak measuring device 2 of the present embodiment, the pipes 10A and 10A constituting the device are used without using the master as in the prior art.
The pressure leak measurement is performed by detecting the differential pressure between an independent closed space formed by closing a part 12B of B, 12A and 12B with an electromagnetic opening / closing valve 40. Therefore, without changing the configuration of the pressure leak measuring device 2, the pressure leak measuring device can perform the differential pressure measurement on many kinds of objects to be measured W, and can perform the pressure leak measuring at low cost.

【0023】本実施例は主として請求項2の発明に対応
するものであるが、電磁弁20,30,40の全てが必
須のものではなく、電磁弁20,30のいずれかを省略
することも可能である。また、請求項2の発明とは対応
しないが、電磁弁40を廃して電磁弁20,30のみで
も、同様の測定を行うことができる。本実施例において
は、加圧気体としてエアコンプレッサ4から供給される
圧縮空気を使用しているが、その他の気体を用いても良
い。また、本実施例では、開閉弁として電磁ソレノイド
によって二つの弁室を交互に配管に接続する電磁開閉
(方向)弁20,30,40を使用しているが、開閉弁
としてはこの他にも種々の形式の弁を使用することがで
きる。さらに、差圧センサ8としても、ダイヤフラム
式,ベローズ式等を始めとして、種々の方式の差圧検出
器を用いることが可能である。圧力洩れ測定装置のその
他の部分の構成,形状,大きさ,材料,数,接続関係等
についても、本実施例に限定されるものではない。
Although this embodiment mainly corresponds to the invention of claim 2, not all of the solenoid valves 20, 30, 40 are indispensable, and either one of the solenoid valves 20, 30 may be omitted. It is possible. Although not corresponding to the second aspect of the invention, the same measurement can be performed with only the solenoid valves 20 and 30 without the solenoid valve 40. Although compressed air supplied from the air compressor 4 is used as the pressurized gas in this embodiment, other gas may be used. Further, in the present embodiment, as the opening / closing valve, the electromagnetic opening / closing (direction) valves 20, 30 and 40 that alternately connect the two valve chambers to the pipe by the electromagnetic solenoid are used. Various types of valves can be used. Further, as the differential pressure sensor 8, it is possible to use various types of differential pressure detectors including a diaphragm type and a bellows type. The configuration, shape, size, material, number, connection relationship, etc. of the other parts of the pressure leak measuring device are not limited to those in this embodiment.

【0024】実施例2 次に、本発明を具現化した実施例2について、図3及び
図4を参照して説明する。まず、本実施例の圧力洩れ測
定装置の基本的構成及び操作について図3を参照して説
明する。図3(A)は本実施例の圧力洩れ測定装置52
の基本的構成を示すブロック図であり、図3(B)は開
閉弁の開閉を示すチャート図である。図3(A)に示さ
れる圧力洩れ測定装置52は、実施例1と同様に、加圧
気体源54と、加圧気体源54を被測定物W及び差圧検
出器58と接続する配管系、及び配管系に設けられた開
閉弁70,80,90,100を中心として構成されて
いる。これらのうち、加圧気体源54,被測定物W,差
圧検出器58及び開閉弁70,80,90の接続関係
は、実施例1と同様である。実施例1と異なるのは、独
立した密閉空間となる配管62B,64Bと被測定物W
とが配管62C,62Dによって接続され、さらに配管
62Cと62Dの間に開閉弁100が設けられている点
である。なお配管62B,64B又は62Cのいずれか
に、エアチャンバACを接続することが好ましい。この
エアチャンバACが接続されていると、第1実施例と同
様、検出感度が向上する。本実施例は主として請求項3
の発明に対応するものであり、圧力洩れ測定装置52に
おいては、これらの配管62C,62Dの存在によって
被測定物W内の圧力がより速く測定圧力に到達するとと
もに、差圧測定の対象となる配管64Bと被測定物Wと
の間での圧力平衡がより短時間で達成される。
Second Embodiment Next, a second embodiment embodying the present invention will be described with reference to FIGS. 3 and 4. First, the basic configuration and operation of the pressure leak measuring device of this embodiment will be described with reference to FIG. FIG. 3A shows a pressure leak measuring device 52 of this embodiment.
3B is a block diagram showing the basic configuration of FIG. 3, and FIG. 3B is a chart diagram showing opening / closing of the on-off valve. The pressure leak measuring device 52 shown in FIG. 3A has a pressurized gas source 54 and a piping system for connecting the pressurized gas source 54 to the object to be measured W and the differential pressure detector 58, as in the first embodiment. , And the on-off valves 70, 80, 90, 100 provided in the piping system. Among these, the connection relationship among the pressurized gas source 54, the measured object W, the differential pressure detector 58, and the open / close valves 70, 80, 90 is the same as that in the first embodiment. The difference from the first embodiment is that the pipes 62B, 64B and the object to be measured W which are independent closed spaces are provided.
Are connected by pipes 62C and 62D, and an on-off valve 100 is provided between the pipes 62C and 62D. The air chamber AC is preferably connected to any of the pipes 62B, 64B or 62C. When this air chamber AC is connected, the detection sensitivity is improved as in the first embodiment. The present embodiment mainly describes claim 3.
In the pressure leak measuring device 52, the pressure inside the object to be measured W reaches the measuring pressure faster due to the presence of these pipes 62C and 62D, and it becomes an object of differential pressure measurement. The pressure equilibrium between the pipe 64B and the object to be measured W is achieved in a shorter time.

【0025】かかる構成の圧力洩れ測定装置52におけ
る測定では、図3(B)に示されるように、まず開閉弁
70,80,90,100が全て開けられ、加圧気体源
54から被測定物W及び配管62B,…内に加圧気体が
導入される。続いて開閉弁70,80,90が閉じら
れ、一定時間だけ開閉弁100のみが開状態とされて、
被測定物Wと配管62B,62C,64Bとの気圧の平
衡が図られる。その後、開閉弁100も閉じられて、開
閉弁90,100と差圧検出器8で挟まれた配管62
B,62C,64Bが独立した密閉空間とされる。この
密閉空間内の気圧と被測定物W内の気圧との差圧が差圧
検出器58において測定され、気体洩れがあれば気体洩
れ分だけの差圧が検出される。ここで、実施例1と異な
るのは、密閉空間62B,62C,64Bと被測定物W
との気圧の平衡が、両者を配管62Dで連通させること
によって行われる点である。このように、密閉空間とな
る部分と被測定物Wとを直接連通させることができるた
め、両者の圧力差を小さくでき、配管内の圧力をより速
く安定させることができる。
In the measurement by the pressure leakage measuring device 52 having such a structure, as shown in FIG. 3B, first, all the on-off valves 70, 80, 90, 100 are opened, and the pressurized gas source 54 is used to measure the object to be measured. Pressurized gas is introduced into W and the pipes 62B, .... Subsequently, the open / close valves 70, 80, 90 are closed, and only the open / close valve 100 is opened for a certain period of time.
An equilibrium of the atmospheric pressure between the measured object W and the pipes 62B, 62C, 64B is achieved. After that, the opening / closing valve 100 is also closed, and the pipe 62 sandwiched between the opening / closing valves 90 and 100 and the differential pressure detector 8 is inserted.
B, 62C and 64B are independent closed spaces. The differential pressure between the atmospheric pressure in the closed space and the atmospheric pressure in the object to be measured W is measured by the differential pressure detector 58, and if there is a gas leak, the differential pressure corresponding to the gas leak is detected. Here, the difference from the first embodiment is that the closed spaces 62B, 62C, 64B and the object to be measured W are
This is the point where the equilibrium of the atmospheric pressures of and is performed by connecting the two with the pipe 62D. In this way, since the portion to be the closed space and the object to be measured W can be directly communicated with each other, the pressure difference between the two can be reduced and the pressure in the pipe can be stabilized more quickly.

【0026】次に、圧力洩れ測定装置52のより具体的
な構成及び測定の手順について、図4を参照して説明す
る。図4(A)は圧力洩れ測定装置52の具体的構成を
示す配管図であり、図4(B)は圧力洩れ測定の手順を
示すチャート図である。圧力洩れ測定装置52において
も加圧気体源としてエアコンプレッサ54を用いてお
り、圧縮空気中の粉塵等を除去するエアフィルタ56を
介して、配管60Aによって電磁方向弁70に接続され
ている。以下、配管60B,60C,60D,60E,
62A,62B,64A,64B,電磁開閉弁80,9
0,差圧センサ58及び被測定物Wの接続関係は、実施
例1と同様である。これに加えて圧力洩れ測定装置52
では、接続部66Cにおいて配管62Cが配管62B,
64Bに接続されている。配管62Cは電磁開閉弁10
0に接続され、電磁開閉弁100の他端は配管62Dを
介して被測定物Wに接続されている。なお、配管62D
と配管60Eの被測定物Wへの接続位置は異なってい
る。配管62CにエアチャンバACを接続することで、
検出感度を向上させることが好ましい。
Next, a more specific structure of the pressure leak measuring device 52 and a measuring procedure will be described with reference to FIG. FIG. 4 (A) is a piping diagram showing a specific configuration of the pressure leak measuring device 52, and FIG. 4 (B) is a chart diagram showing the procedure of pressure leak measuring. The pressure leak measuring device 52 also uses an air compressor 54 as a source of pressurized gas, and is connected to the electromagnetic directional valve 70 by a pipe 60A via an air filter 56 that removes dust and the like in the compressed air. Hereinafter, the pipes 60B, 60C, 60D, 60E,
62A, 62B, 64A, 64B, solenoid on-off valves 80, 9
The connection relationship between 0, the differential pressure sensor 58, and the object to be measured W is the same as that in the first embodiment. In addition to this, the pressure leak measuring device 52
Then, at the connecting portion 66C, the pipe 62C is connected to the pipe 62B,
It is connected to 64B. The pipe 62C is the solenoid valve 10.
0, and the other end of the electromagnetic on-off valve 100 is connected to the DUT W through a pipe 62D. Note that the pipe 62D
And the connection position of the pipe 60E to the measured object W is different. By connecting the air chamber AC to the pipe 62C,
It is preferable to improve the detection sensitivity.

【0027】電磁方向弁70は、実施例1の電磁方向弁
20と異なり、二つの弁室74A,74Bを有してい
る。電磁ソレノイド72の非作動時には、スプリング7
6の付勢力によって、弁室74Bが配管60A及び配管
60Bに接続される。すなわち、図4(A)に示される
状態となる。このとき、配管60Aは閉状態のポートに
接続され、一方配管60Bは排気消音器78に通ずるポ
ートに接続された状態となる。これによって、配管60
B以降の配管及び被測定物W,差圧検出器58内に残留
していた圧縮空気が、排気消音器78から大気中に放出
される。一方、図示しない制御ユニットからの制御信号
によって電磁ソレノイド72が励磁されると、弁室74
A,74Bがスプリング76の付勢力に抗して移動し、
弁室74Aが配管60Aに接続される。これによって、
配管60Aと配管60Bが接続され、エアコンプレッサ
54から圧縮空気が配管系に供給される。なお、電磁開
閉弁80,90,100の構造は、実施例1の電磁開閉
弁30,40と同様である。
Unlike the electromagnetic directional valve 20 of the first embodiment, the electromagnetic directional valve 70 has two valve chambers 74A and 74B. When the electromagnetic solenoid 72 is inactive, the spring 7
The valve chamber 74B is connected to the pipe 60A and the pipe 60B by the urging force of 6. That is, the state shown in FIG. At this time, the pipe 60A is connected to the closed port, while the pipe 60B is connected to the port communicating with the exhaust silencer 78. This allows the pipe 60
The compressed air remaining in the piping after B, the object to be measured W, and the differential pressure detector 58 is discharged from the exhaust silencer 78 into the atmosphere. On the other hand, when the electromagnetic solenoid 72 is excited by a control signal from a control unit (not shown), the valve chamber 74
A and 74B move against the urging force of the spring 76,
The valve chamber 74A is connected to the pipe 60A. by this,
The pipe 60A and the pipe 60B are connected, and compressed air is supplied from the air compressor 54 to the pipe system. The structure of the electromagnetic on-off valves 80, 90, 100 is the same as that of the electromagnetic on-off valves 30, 40 of the first embodiment.

【0028】かかる構成を有する圧力洩れ測定装置52
による圧力洩れ測定の各段階について、図4(A)及び
図4(B)を参照しつつ説明する。ここで、Pm2は圧力
センサ68Bによって測定される圧力であり、圧力PX2
は圧力センサ68Aによって測定される圧力を示し、P
W2は被測定物W内の圧力を示す。まず、加圧段階として
所定時間T4の間、開閉弁70,80,90,100が
全て開状態(弁室74A,84A,94A,104Aが
接続された状態)となり、エアコンプレッサ4から被測
定物W及び各配管内に圧縮空気が導入される。ここで、
圧力洩れ測定装置52においては、配管60C,60
D,60Eからのみならず、配管62A,62B,62
C,62Dからも圧縮空気が供給されるため、被測定物
W内の圧力をより速く測定圧力に到達させることができ
る。続いて電磁開閉弁80,90が閉じられ、さらに電
磁方向弁70が切替えられてエアコンプレッサ54から
の圧縮空気の供給が遮断される。なお、図4(B)にお
いては電磁方向弁70と電磁開閉弁80,90とを同時
に切り替えるように示されているが、実際には完全に同
時ではなく、まず電磁開閉弁80,90を閉じて配管系
の密閉を確保してから、電磁方向弁70が切替えられ
る。これによって、被測定物W及び配管60D,…,6
2B内の圧力が均等化され、この所定時間T5の平衡段
階によって、圧力Pm2とPX2とが平衡に達する。
Pressure leak measuring device 52 having such a configuration
Each stage of the pressure leak measurement by the method will be described with reference to FIGS. 4 (A) and 4 (B). Here, P m2 is the pressure measured by the pressure sensor 68B, and the pressure P X2
Indicates the pressure measured by the pressure sensor 68A, and P
W2 indicates the pressure inside the object to be measured W. First, the opening / closing valves 70, 80, 90, 100 are all opened (the valve chambers 74A, 84A, 94A, 104A are connected) for a predetermined time T4 as a pressurizing step, and the object to be measured is discharged from the air compressor 4. Compressed air is introduced into W and each pipe. here,
In the pressure leak measuring device 52, the pipes 60C, 60
Not only from D and 60E, but also from piping 62A, 62B and 62
Since compressed air is also supplied from C and 62D, the pressure in the object to be measured W can reach the measured pressure faster. Subsequently, the electromagnetic on-off valves 80 and 90 are closed, and the electromagnetic directional valve 70 is switched to shut off the supply of compressed air from the air compressor 54. In FIG. 4B, the electromagnetic directional valve 70 and the electromagnetic opening / closing valves 80, 90 are shown to be switched at the same time. However, in reality, they are not completely simultaneous, and the electromagnetic opening / closing valves 80, 90 are first closed. After ensuring the airtightness of the piping system, the electromagnetic directional valve 70 is switched. As a result, the DUT W and the pipes 60D, ..., 6
The pressure in 2B is equalized, and the pressure P m2 and P X2 reach equilibrium by the equilibrium stage of this predetermined time T5.

【0029】ここで、圧力洩れ測定装置52において
は、配管62C,62Dがあるために、差圧測定の対象
となる配管64Bと被測定物Wとの間での圧力平衡が速
く達成される。なお、この平衡段階において圧力センサ
68A,68Bによる測定圧力PX2,Pm2が降下する場
合には、被測定物Wあるいは配管系のどこかに大きな洩
れがあると判断して、測定を中止する。かかる平衡段階
の後に、開閉弁100が閉じられて配管62B,62
C,64Bが独立した密閉空間とされ、差圧センサ58
によって被測定物Wと配管62B,62C,64Bの差
圧が測定される。かかる検出段階において、被測定物W
からの空気洩れがある場合には、圧力Pm2は変化しない
のに対して圧力PX2は低下するため、差圧の変化として
表れる。これに対して、被測定物Wからの空気洩れがな
い場合には、圧力PX2は圧力P m2と同じ値に保たれるた
め、差圧センサ58で測定される差圧はゼロとなる。従
って、差圧センサ58からの出力信号を図示しない制御
ユニットで解析することによって、被測定物Wからの空
気洩れの有無とその大きさを測定できる。
In the pressure leak measuring device 52,
Is the target of differential pressure measurement because there are pipes 62C and 62D.
The pressure equilibrium between the pipe 64B and the object to be measured W becomes fast.
Achieved. Note that the pressure sensor
Measured pressure P by 68A, 68BX2, Pm2Place where
If there is a large leak in the measured object W or somewhere in the piping system,
If there is any, stop the measurement. Such equilibration stage
After that, the on-off valve 100 is closed and the pipes 62B, 62
C and 64B are independent closed spaces, and the differential pressure sensor 58
The difference between the measured object W and the pipes 62B, 62C, 64B
The pressure is measured. At the detection stage, the object to be measured W
If there is air leakage from them2Does not change
Against pressure PX2Will decrease, so
appear. On the other hand, there is no air leakage from the DUT W.
If not, pressure PX2Is the pressure P m2Is kept at the same value as
Therefore, the differential pressure measured by the differential pressure sensor 58 becomes zero. Obedience
The output signal from the differential pressure sensor 58 is not shown in the figure.
By analyzing with the unit, the sky from the measured object W
It is possible to measure the presence or absence of air leak and its size.

【0030】測定終了後は、開閉弁70,80,90,
100の電磁ソレノイド72,…,102の作動が解除
されて弁室74B,…,104Aが各配管に接続され、
被測定物W及び各配管内の圧縮空気が排気消音器28か
ら排出される。このように本実施例の圧力洩れ測定装置
52では、配管60C,60D,60Eと配管62A,
62B,62C,62Dの二系統でエアコンプレッサ5
4から被測定物Wへ圧縮空気を供給することによって、
被測定物W内の圧力をより速く測定圧力に到達させるこ
とができる。また、独立した密閉空間となる配管62
B,64Bと被測定物Wとが配管62C,配管62Dで
接続されているため、密閉空間62B,64Bと被測定
物Wとの圧力平衡がより短時間で達成される。このよう
にして、短時間で高精度の圧力洩れ測定を行うことがで
きる圧力洩れ測定装置となる。
After the measurement, the on-off valves 70, 80, 90,
The electromagnetic solenoids 72, ..., 102 of 100 are released from operation and the valve chambers 74B, ..., 104A are connected to the respective pipes,
The object to be measured W and the compressed air in each pipe are discharged from the exhaust silencer 28. As described above, in the pressure leak measuring device 52 of the present embodiment, the pipes 60C, 60D and 60E and the pipe 62A,
Air compressor 5 with two systems of 62B, 62C and 62D
By supplying compressed air from 4 to the object to be measured W,
The pressure in the object to be measured W can reach the measured pressure faster. In addition, a pipe 62 that becomes an independent closed space
Since B and 64B and the measured object W are connected by the pipes 62C and 62D, the pressure equilibrium between the closed spaces 62B and 64B and the measured object W is achieved in a shorter time. In this way, the pressure leak measuring device is capable of performing highly accurate pressure leak measurement in a short time.

【0031】実施例3 次に、本発明を具現化した実施例3について、図5〜図
7を参照して説明する。まず、本実施例の圧力洩れ測定
装置の基本的構成及び操作について図5を参照して説明
する。図5(A)は本実施例の圧力洩れ測定装置112
の基本的構成を示すブロック図であり、図5(B)は開
閉弁の開閉を示すチャート図である。図5(A)に示さ
れる圧力洩れ測定装置112も、実施例1,2と同様
に、加圧気体源114,差圧検出器118,これらと被
測定物Wを接続する配管系及び開閉弁130,140を
中心として構成されている。但し、本実施例では、これ
らの接続の順序及び配管系の構成が実施例1,2とはか
なり異なっている。本実施例においては、閉ループ状に
形成された配管系の一部124Bによって、独立した密
閉空間が構成される。さらに、この独立した密閉空間と
なる配管124Bが、加圧気体源114に対して被測定
物Wよりも後方(二次側)に接続されている点が特徴で
ある。かかる構成によって、本実施例の圧力洩れ測定装
置112においては、被測定物W内の圧力がより速く測
定圧力に到達するとともに、差圧測定の対象となる配管
124Bと被測定物Wとの気圧差がなくなり、圧力平衡
が速く達成される。
Third Embodiment Next, a third embodiment embodying the present invention will be described with reference to FIGS. First, the basic configuration and operation of the pressure leak measuring device of this embodiment will be described with reference to FIG. FIG. 5A shows a pressure leak measuring device 112 of this embodiment.
5B is a block diagram showing the basic configuration of FIG. 5B, and FIG. 5B is a chart showing the opening and closing of the on-off valve. Similarly to the first and second embodiments, the pressure leak measuring device 112 shown in FIG. 5A also has a pressurized gas source 114, a differential pressure detector 118, a piping system and an opening / closing valve for connecting these to the object W to be measured. It is configured around 130 and 140. However, in this embodiment, the order of these connections and the configuration of the piping system are quite different from those in the first and second embodiments. In this embodiment, an independent closed space is formed by the part 124B of the pipe system formed in the closed loop shape. Further, the pipe 124 </ b> B, which is an independent closed space, is connected to the pressurized gas source 114 rearward (secondary side) of the object W to be measured. With this configuration, in the pressure leak measuring device 112 of the present embodiment, the pressure in the object to be measured W reaches the measured pressure faster, and the pressure between the pipe 124B, which is the object of differential pressure measurement, and the object to be measured W. There is no difference and pressure equilibration is achieved quickly.

【0032】具体的には、図5(A)に示されるよう
に、加圧気体源114は、配管120A,開閉弁13
0,配管120Bを介して被測定物Wに接続されてい
る。被測定物Wの配管120Bの接続部分と対向する位
置には、配管122Aが接続され、この配管122Aか
らは配管122B及び配管124Aが分岐している。配
管122Bは差圧検出器118の測定部の一方に接続さ
れ、配管124Aは開閉弁140,配管124Bを介し
て差圧検出器118の他方の測定部に接続されている。
このようにして、配管122B,差圧検出器118,配
管124B,開閉弁140,配管124Aによって、差
圧検出のための閉ループ状の配管系が形成されている。
この実施例の場合も、配管124Bにエアチャンバを接
続することが好ましく、エアチャンバACを接続する
と、検出感度は向上する。
Specifically, as shown in FIG. 5A, the pressurized gas source 114 includes a pipe 120A and an opening / closing valve 13.
0, connected to the object to be measured W via a pipe 120B. A pipe 122A is connected to the measured object W at a position facing the connecting portion of the pipe 120B, and a pipe 122B and a pipe 124A are branched from the pipe 122A. The pipe 122B is connected to one of the measuring units of the differential pressure detector 118, and the pipe 124A is connected to the other measuring unit of the differential pressure detector 118 via the on-off valve 140 and the pipe 124B.
In this way, the pipe 122B, the differential pressure detector 118, the pipe 124B, the on-off valve 140, and the pipe 124A form a closed-loop pipe system for differential pressure detection.
Also in this embodiment, it is preferable to connect the air chamber to the pipe 124B, and if the air chamber AC is connected, the detection sensitivity is improved.

【0033】かかる構成の圧力洩れ測定装置112にお
ける測定では、図5(B)に示されるように、まず開閉
弁130,140が共に開けられ、加圧気体源114か
ら被測定物W内に加圧気体が導入される。加圧気体は、
被測定物Wの二次側に接続された配管122Aから、さ
らに閉ループ状配管122B,124A,124B内に
導入される。続いて開閉弁130が閉じられ、一定時間
だけ開閉弁140のみが開状態とされて、被測定物Wと
閉ループ状配管122B,…との気圧の平衡が図られ
る。その後、開閉弁140が閉じられて、開閉弁140
と差圧検出器118で挟まれた配管124Bが独立した
密閉空間とされる。この密閉空間内の気圧と被測定物W
内の気圧との差圧が差圧検出器118において測定さ
れ、気体洩れがあれば気体洩れ分だけの差圧が検出され
る。
In the measurement by the pressure leak measuring device 112 having such a configuration, as shown in FIG. 5B, first, the on-off valves 130 and 140 are both opened, and the pressurized gas source 114 is applied to the object to be measured W. Pressurized gas is introduced. The pressurized gas is
From the pipe 122A connected to the secondary side of the object to be measured W, it is further introduced into the closed loop pipes 122B, 124A, 124B. Then, the on-off valve 130 is closed, and only the on-off valve 140 is opened for a certain period of time to balance the atmospheric pressures of the object W to be measured and the closed loop pipes 122B, .... After that, the on-off valve 140 is closed and the on-off valve 140
The pipe 124B sandwiched between the differential pressure detector 118 and the differential pressure detector 118 is an independent closed space. Atmospheric pressure in this closed space and object to be measured W
The differential pressure from the internal pressure is measured by the differential pressure detector 118, and if there is a gas leak, the differential pressure corresponding to the gas leak is detected.

【0034】次に、圧力洩れ測定装置112のより具体
的な構成と測定の手順について、図6を参照して説明す
る。図6(A)は圧力洩れ測定装置112の具体的構成
を示す配管図であり、図6(B)は圧力洩れ測定の手順
を示すチャート図である。圧力洩れ測定装置112にお
いても加圧気体源としてエアコンプレッサ114を用
い、配管126Aには、圧縮空気中の粉塵等を除去する
エアフィルタ116が取り付けられている。配管126
Aは、配管126B及び配管126Cに分岐しており、
配管126Bは圧力レギュレータ150を介して電磁方
向弁170の一方の入力ポートに接続されている。配管
126Bには、圧力レギュレータ150による圧力を測
定するための圧力ゲージ156が取り付けられており、
圧力レギュレータ150による圧力は調節ねじ152に
よって調節される。配管126Cは、増圧レギュレータ
160を介して、電磁方向弁170の他方の入力ポート
に接続されている。増圧レギュレータ160は、供給さ
れた圧縮空気の圧力を圧力レギュレータ150よりも高
圧にするように調節されている。配管126Cには、増
圧レギュレータ160による圧力を測定するための圧力
ゲージ162が取り付けられている。
Next, a more specific structure of the pressure leak measuring device 112 and a measuring procedure will be described with reference to FIG. FIG. 6 (A) is a piping diagram showing a specific configuration of the pressure leak measuring device 112, and FIG. 6 (B) is a chart diagram showing a procedure of pressure leak measuring. Also in the pressure leak measuring device 112, the air compressor 114 is used as a pressurized gas source, and an air filter 116 for removing dust and the like in the compressed air is attached to the pipe 126A. Plumbing 126
A is branched into a pipe 126B and a pipe 126C,
The pipe 126B is connected to one input port of the electromagnetic directional valve 170 via the pressure regulator 150. A pressure gauge 156 for measuring the pressure by the pressure regulator 150 is attached to the pipe 126B,
The pressure by the pressure regulator 150 is adjusted by the adjusting screw 152. The pipe 126C is connected to the other input port of the electromagnetic directional valve 170 via the pressure boosting regulator 160. The booster regulator 160 is adjusted so that the pressure of the supplied compressed air is higher than that of the pressure regulator 150. A pressure gauge 162 for measuring the pressure by the pressure boosting regulator 160 is attached to the pipe 126C.

【0035】電磁方向弁170の出力ポートには配管1
26Dが接続されており、以下、電磁方向弁180,配
管120A,電磁開閉弁130,配管120Bを介し
て、被測定物Wに接続されている。被測定物Wの配管1
20Bの接続部に対向する位置には、配管122Aが接
続されており、この配管122Aに配管122B以下の
閉ループ配管系が接続されている。なお、配管122A
の途中には、圧力検出センサ164が取り付けられてい
る。閉ループ配管系は、差圧センサ118の一方に接続
された配管122Bと、差圧センサ118の他方に接続
された配管124B、そして配管124Bから電磁開閉
弁140,電磁方向弁190を介して配管122Bに接
続された配管124AIによって構成されている。配管
124BにエアチャンバACを接続するようにしてもよ
い。電磁方向弁170,180,190の構造は前述の
電磁方向弁20等と同様であり、電磁開閉弁130,1
40の構造は電磁開閉弁30等と同様である。
Piping 1 is provided at the output port of the electromagnetic directional valve 170.
26D is connected to the object to be measured W through the electromagnetic directional valve 180, the pipe 120A, the electromagnetic opening / closing valve 130, and the pipe 120B. Piping 1 of the object to be measured W
A pipe 122A is connected to a position facing the connecting portion of 20B, and a closed loop pipe system including a pipe 122B and below is connected to the pipe 122A. Note that the pipe 122A
A pressure detection sensor 164 is attached midway. The closed loop piping system includes a pipe 122B connected to one side of the differential pressure sensor 118, a pipe 124B connected to the other side of the differential pressure sensor 118, and a pipe 122B from the pipe 124B via an electromagnetic opening / closing valve 140 and an electromagnetic directional valve 190. It is constituted by a pipe 124AI connected to. The air chamber AC may be connected to the pipe 124B. The structure of the electromagnetic directional valves 170, 180 and 190 is the same as that of the electromagnetic directional valve 20 and the like described above.
The structure of 40 is the same as that of the solenoid on-off valve 30 and the like.

【0036】かかる構成を有する圧力洩れ測定装置11
2による圧力洩れ測定の各段階について、図6(A)及
び図6(B)を参照しつつ説明する。なお、Pm3は配管
124Bにおける気圧を表し、圧力PX3は圧力センサ1
64によって測定される気圧を、PW3は被測定物W内の
気圧を示す。図6(B)に示されるように、まず、所定
時間T7の加圧操作が実行される。最初に予備加圧とし
て、所定時間ΔT7の間、電磁方向弁170及び180
が電磁ソレノイド172,182の励磁状態(弁室17
4A,184Aが接続された状態)となる。これによっ
て配管126Bは閉状態となり、配管126Cが配管1
26Dと連通する。また、電磁方向弁180は開状態と
なる。一方、電磁開閉弁130,140及び電磁方向弁
190は電磁ソレノイドが非励磁であり、いずれも開状
態となっている。
Pressure leak measuring device 11 having such a configuration
Each step of pressure leak measurement according to No. 2 will be described with reference to FIGS. 6 (A) and 6 (B). Note that P m3 represents the atmospheric pressure in the pipe 124B, and the pressure P X3 is the pressure sensor 1.
P W3 indicates the atmospheric pressure measured by 64, and P W3 indicates the atmospheric pressure inside the object to be measured W. As shown in FIG. 6B, first, the pressurizing operation for a predetermined time T7 is executed. First, as pre-pressurization, the electromagnetic directional valves 170 and 180 are operated for a predetermined time ΔT7.
Is the excited state of the electromagnetic solenoids 172, 182 (valve chamber 17
4A and 184A are connected). As a result, the pipe 126B is closed, and the pipe 126C is connected to the pipe 1
It communicates with 26D. Further, the electromagnetic directional valve 180 is opened. On the other hand, the electromagnetic on-off valves 130 and 140 and the electromagnetic directional valve 190 are in the open state because the electromagnetic solenoids are not excited.

【0037】従って、エアコンプレッサ114から供給
された圧縮空気は、増圧レギュレータ160によって高
圧に調節されて、配管120A,120Bを介して被測
定物W内に供給される。そして、さらに配管122Aを
介して配管122B以下の閉ループ配管系に導入され
る。所定時間ΔT7の経過後、電磁方向弁170が切替
えられて配管126Cが閉じられ、配管126Bが配管
126Dと連通する。これによって、今度は圧力レギュ
レータ150で測定圧力に調節された圧縮空気が、被測
定物W及び配管系に供給される。このように、最初に測
定圧力より高圧の圧縮空気を、次に測定圧力の圧縮空気
を供給するという二段階の加圧を行うことによって、圧
縮空気が被測定物W内に導入される際の温度変化等によ
る圧力変動を最小限に抑えることができる。また、圧縮
空気が被測定物Wを経て配管122B以下の閉ループ配
管系に供給されることによって、両者の圧力差が解消さ
れる。
Therefore, the compressed air supplied from the air compressor 114 is adjusted to a high pressure by the pressure boosting regulator 160 and supplied into the object to be measured W through the pipes 120A and 120B. Then, it is further introduced into the closed loop piping system below the piping 122B via the piping 122A. After the elapse of the predetermined time ΔT7, the electromagnetic directional valve 170 is switched, the pipe 126C is closed, and the pipe 126B communicates with the pipe 126D. As a result, the compressed air, which has been adjusted to the measurement pressure by the pressure regulator 150, is supplied to the object to be measured W and the piping system. In this way, when compressed air having a pressure higher than the measurement pressure is supplied first, and then compressed air having a measurement pressure is supplied, the compressed air is introduced into the object W to be measured. It is possible to minimize pressure fluctuations due to temperature changes and the like. Further, the compressed air is supplied to the closed loop piping system below the piping 122B through the object to be measured W, so that the pressure difference between the two is eliminated.

【0038】かかる加圧操作が時間T7の間行われた
後、平衡操作が行われる。すなわち、電磁方向弁180
及び電磁開閉弁130が切替えられて、エアコンプレッ
サ114からの圧縮空気の供給が遮断される。なお、図
6(B)では電磁弁180と130とを同時に切り替え
るように示されているが、実際には圧縮空気が逃げるの
を防止するために、電磁開閉弁180の切替えが僅かに
遅れて行われる。一方、電磁開閉弁140,電磁方向弁
190は開状態のままとされ、被測定物Wと閉ループ配
管系との連通が保たれる。この状態(零平衡状態)が所
定時間ΔT8だけ維持されることによって、被測定物W
及び閉ループ配管系内の圧力がより均等化されて安定す
る。かかる零平衡操作の後、電磁開閉弁140及び電磁
方向弁190が切替えられて、弁室144Aと弁室19
4Aが配管に接続された状態となる。このときもまず電
磁開閉弁140が閉じ、次に電磁方向弁190が切替え
られる。この結果、配管124AIと配管124Bの連
通が遮断され、電磁開閉弁140と差圧センサ118に
挟まれた配管124Bが独立した密閉空間となる。これ
に伴って、電磁開閉弁140と電磁方向弁190に挟ま
れた配管内の空気は、電磁方向弁190の排気消音器1
98から大気中に排出される。
After the pressurizing operation is performed for the time T7, the equilibrium operation is performed. That is, the electromagnetic directional valve 180
Also, the electromagnetic on-off valve 130 is switched to shut off the supply of compressed air from the air compressor 114. Although FIG. 6B shows that the solenoid valves 180 and 130 are switched at the same time, in actuality, switching of the solenoid on-off valve 180 is slightly delayed to prevent compressed air from escaping. Done. On the other hand, the electromagnetic opening / closing valve 140 and the electromagnetic directional valve 190 are left in the open state, and the communication between the DUT W and the closed loop piping system is maintained. By maintaining this state (zero equilibrium state) for a predetermined time ΔT8, the measured object W
And the pressure in the closed loop piping system is more equalized and stabilized. After such a zero balance operation, the solenoid on-off valve 140 and the solenoid directional valve 190 are switched, and the valve chamber 144A and the valve chamber 19 are switched.
4A is connected to the pipe. Also at this time, the electromagnetic on-off valve 140 is first closed, and then the electromagnetic directional valve 190 is switched. As a result, the communication between the pipe 124AI and the pipe 124B is cut off, and the pipe 124B sandwiched between the electromagnetic opening / closing valve 140 and the differential pressure sensor 118 becomes an independent closed space. Along with this, the air in the pipe sandwiched between the electromagnetic on-off valve 140 and the electromagnetic directional valve 190 is the exhaust silencer 1 of the electromagnetic directional valve 190.
Emitted from 98 into the atmosphere.

【0039】この弁操作から所定時間(=T8−ΔT
8)経過後に、差圧検出段階に入る。このような待ち時
間(T8−ΔT8)を設けるのは、電磁開閉弁140と
電磁方向弁190の切換え時に一時的に生ずる微小な差
圧を解消させるためである。差圧検出段階においては、
所定の検出時間T9経過後の差圧センサ118の測定値
(出力電圧)が、図示しない制御ユニットに入力され
る。そして、平衡段階から検出段階に切り替わった時点
における差圧センサ118の出力電圧を基準として、予
め求められた計算式から圧力洩れ量を算出して出力す
る。測定終了後は、図6(B)に示されるように、電磁
開閉弁130,140及び電磁方向弁190の電磁ソレ
ノイドの励磁が解除されて連通状態とされ、被測定物W
及び各配管内の圧縮空気が電磁方向弁180の排気消音
器186から排出される。
A predetermined time from this valve operation (= T8-ΔT
8) After the lapse of time, the differential pressure detecting step is started. The reason for providing such a waiting time (T8−ΔT8) is to eliminate a minute differential pressure that is temporarily generated when the electromagnetic switching valve 140 and the electromagnetic directional valve 190 are switched. In the differential pressure detection stage,
The measured value (output voltage) of the differential pressure sensor 118 after the elapse of the predetermined detection time T9 is input to a control unit (not shown). Then, with the output voltage of the differential pressure sensor 118 at the time of switching from the equilibrium stage to the detection stage as a reference, the pressure leakage amount is calculated and output from a previously calculated formula. After the measurement is completed, as shown in FIG. 6B, the electromagnetic solenoids of the electromagnetic opening / closing valves 130 and 140 and the electromagnetic directional valve 190 are deenergized to be in the communication state, and the measured object W
And the compressed air in each pipe is discharged from the exhaust silencer 186 of the electromagnetic directional valve 180.

【0040】次に、圧力洩れ測定装置112による具体
的な測定結果について、図7を参照して説明する。図7
は、本実施例の圧力洩れ測定装置112による測定にお
ける圧力と差圧の変化を示すグラフである。圧力は図6
(A)の圧力センサ164で測定される圧力であり、差
圧は差圧センサ118で測定される差圧である。なお、
この差圧は、被測定物W側の圧力が高く、密封配管側の
圧力が低い場合を正とし、その反対のときを負としてい
る。図7に示されるように、前述した予備加圧段階にお
いては測定圧力より高圧に調節された圧縮空気が供給さ
れるため、圧力センサ164の測定値は、一旦測定圧力
を越える。予備加圧終了後には測定圧力に調節された圧
縮空気が供給されるため、圧力値は測定圧力まで下がっ
て安定する。この予備加圧の過程で、閉ループ配管の配
管122B側と、二つの電磁弁190,140を介する
配管124B側とでは管路抵抗が微妙に異なるため、図
7のように差圧センサ118で差圧が検出される。そこ
で、この現象を利用して、検出される差圧の絶対値が大
きくなるように閉ループ配管の各配管長さを変えたり、
必要なら絞り弁を入れる等することによって、以下の検
出段階における検出感度を向上させることができる。ま
た、この予備加圧段階において所定値以上の圧力変動が
発生した場合には、被測定物に孔が存在する等の異常と
判定して、測定を中断して検査する。
Next, a concrete measurement result by the pressure leak measuring device 112 will be described with reference to FIG. Figure 7
[Fig. 4] is a graph showing changes in pressure and differential pressure in measurement by the pressure leak measuring device 112 of the present embodiment. Figure 6
(A) is the pressure measured by the pressure sensor 164, and the differential pressure is the differential pressure measured by the differential pressure sensor 118. In addition,
This differential pressure is positive when the pressure on the measured object W side is high and low on the sealed pipe side, and negative when the pressure is opposite. As shown in FIG. 7, since compressed air adjusted to a pressure higher than the measured pressure is supplied in the pre-pressurization step described above, the measured value of the pressure sensor 164 once exceeds the measured pressure. After the pre-pressurization is completed, compressed air adjusted to the measurement pressure is supplied, so that the pressure value drops to the measurement pressure and stabilizes. In the process of this preliminary pressurization, since the pipe line resistance is slightly different between the pipe 122B side of the closed loop pipe and the pipe 124B side through the two solenoid valves 190, 140, the differential pressure sensor 118 makes a difference as shown in FIG. The pressure is detected. Therefore, by using this phenomenon, the length of each closed loop pipe can be changed so that the absolute value of the detected differential pressure becomes large,
The detection sensitivity in the following detection steps can be improved by inserting a throttle valve or the like if necessary. If a pressure fluctuation of a predetermined value or more occurs in the preliminary pressurization stage, it is determined that the object to be measured has an abnormality such as a hole, and the measurement is interrupted for inspection.

【0041】続く平衡段階及び検出段階では、被測定物
Wからの圧力洩れがない場合には、圧力センサ164の
測定値は実線で示されるように加圧段階で安定した一定
の圧力に保たれる。ここで、零平衡段階の終了時点にお
いて、図6(B)に示されるように電磁弁140,19
0が同時に切り替えられるために、図7に示されるよう
な差圧が一時的に発生する。この差圧は微小なものであ
り、平衡段階の終了時点では解消されている。一方、圧
力洩れがある場合には、破線で示されるように一定の値
とならずに圧力が降下し続ける。従って、差圧センサ1
18の測定値も、圧力洩れがない場合には実線で示され
るようにゼロを維持し、圧力洩れがある場合には破線で
示されるように一定の値とならずに差圧の絶対値が増加
し続ける。従って、図示しない制御ユニットにおいて、
所定の検出時間T9経過後の差圧センサ118の測定値
(出力電圧)を平衡段階終了時の出力電圧と比較するこ
とによって、被測定物Wからの空気洩れの有無とその大
きさを算出することができる。
In the subsequent equilibrium stage and detection stage, when there is no pressure leak from the object to be measured W, the measurement value of the pressure sensor 164 is maintained at a stable constant pressure in the pressurization stage as shown by the solid line. Be done. Here, at the end of the zero equilibrium stage, as shown in FIG.
Since 0 is switched at the same time, a differential pressure as shown in FIG. 7 temporarily occurs. This differential pressure is so small that it disappears at the end of the equilibration stage. On the other hand, when there is a pressure leak, the pressure does not become a constant value as indicated by the broken line, and the pressure continues to drop. Therefore, the differential pressure sensor 1
The measured values of 18 also maintain zero as indicated by the solid line when there is no pressure leak, and do not become constant as indicated by the broken line when there is pressure leak, and the absolute value of the differential pressure is Continue to increase. Therefore, in the control unit not shown,
By comparing the measured value (output voltage) of the differential pressure sensor 118 after the elapse of the predetermined detection time T9 with the output voltage at the end of the equilibrium stage, the presence or absence of air leakage from the object to be measured W and its magnitude are calculated. be able to.

【0042】以上説明したように、本実施例の圧力洩れ
測定装置112においては、エアコンプレッサ114に
対して被測定物Wの二次側に密閉空間となる閉ループ配
管系を接続しているために、被測定物W内と閉ループ配
管内系の圧力を等しくすることができる。従って、被測
定物Wと配管間の空気の移動が起こらず、圧力が安定す
るため、高精度の測定が可能になるとともに、短時間で
測定することができる。
As described above, in the pressure leak measuring device 112 of this embodiment, the closed loop piping system, which is a closed space, is connected to the secondary side of the object to be measured W with respect to the air compressor 114. The pressures in the object to be measured W and the system in the closed loop pipe can be equalized. Therefore, the movement of air between the object to be measured W and the pipe does not occur, and the pressure is stable, so that highly accurate measurement is possible and the measurement can be performed in a short time.

【0043】実施例4 次に、本発明を具現化した実施例4について、図8及び
図9を参照して説明する。まず、本実施例の圧力洩れ測
定装置の基本的構成と測定の手順について、図8を参照
しつつ説明する。図8(A)に示されるように、本実施
例の圧力洩れ測定装置202は、図6(A)の実施例3
の圧力洩れ測定装置112とほぼ同じである。また、測
定の手順についても、図8(B)に示されるように、実
施例3と同様である。但し、圧力洩れ測定装置202
は、差圧検出器118からの出力信号(出力電圧)を受
ける制御手段として、実施例1〜3と同様の図示しない
制御ユニット以外に、演算処理部210を有している。
この演算処理部210によって、差圧検出器118から
の出力信号を処理して単位時間当たりの差圧の変化を求
め、この変化率から検査段階終了時における差圧の値を
予測する点に特徴がある。すなわち、実施例1〜3のよ
うに、差圧の測定値がある程度安定する所定の検査時間
まで待つ必要がなく、検査の初期において演算処理を行
い結果を予測することによって、極めて短時間に測定を
完了することができる。
Fourth Embodiment Next, a fourth embodiment embodying the present invention will be described with reference to FIGS. 8 and 9. First, the basic configuration of the pressure leak measuring device of the present embodiment and the measurement procedure will be described with reference to FIG. As shown in FIG. 8 (A), the pressure leak measuring device 202 of this embodiment is the same as that of the third embodiment of FIG. 6 (A).
This is almost the same as the pressure leak measuring device 112. The measurement procedure is also the same as in Example 3, as shown in FIG. However, the pressure leak measuring device 202
In addition to the control unit (not shown) similar to the first to third embodiments, the arithmetic processing unit 210 is provided as a control unit that receives the output signal (output voltage) from the differential pressure detector 118.
This arithmetic processing unit 210 processes the output signal from the differential pressure detector 118 to obtain the change in the differential pressure per unit time, and predicts the value of the differential pressure at the end of the inspection stage from this rate of change. There is. That is, unlike Examples 1 to 3, it is not necessary to wait until a predetermined inspection time at which the measured value of the differential pressure becomes stable to some extent, and the calculation processing is performed in the initial stage of the inspection to predict the result, so that the measurement is performed in an extremely short time. Can be completed.

【0044】本実施例の圧力洩れ測定装置202による
具体的な測定結果について、図9を参照して説明する。
図9は、本実施例の圧力洩れ測定装置202による測定
における圧力と差圧の変化を示すグラフである。図9に
示されるように、圧力洩れ測定装置202による測定に
おいても、加圧段階から平衡段階にかけての圧力及び差
圧の経時変化は、図7の実施例3と似たものとなる。本
実施例においても、図7に示される実施例3の場合と同
様に、零平衡後に電磁弁140,190の切替えに伴う
一時的な差圧が発生する。そして、時間ΔT11の零平
衡の後は、被測定物Wからの圧力洩れの有無によって、
図9のようにそれぞれ異なった差圧変化を示す。すなわ
ち、被測定物Wからの圧力洩れがない場合には、実線で
示されるように、所定の平衡時間T11の後は一定の値
に安定する。一方、圧力洩れがある場合には、破線で示
されるように一定の値とならずに差圧の絶対値が増加し
続ける。また、微小な圧力洩れがある場合には、一点鎖
線で示されるように、これらの中間の曲線となる。
Specific measurement results by the pressure leak measuring device 202 of this embodiment will be described with reference to FIG.
FIG. 9 is a graph showing changes in pressure and differential pressure in measurement by the pressure leak measuring device 202 of this embodiment. As shown in FIG. 9, also in the measurement by the pressure leak measuring device 202, the changes with time of the pressure and the differential pressure from the pressurizing stage to the equilibrium stage are similar to those of the third embodiment of FIG. 7. In the present embodiment as well, similar to the case of the third embodiment shown in FIG. 7, a temporary differential pressure is generated after switching the solenoid valves 140 and 190 after zero equilibrium. After the zero equilibrium of time ΔT11, depending on the presence or absence of pressure leak from the object to be measured W,
As shown in FIG. 9, different differential pressure changes are shown. That is, when there is no pressure leak from the object to be measured W, as shown by the solid line, it stabilizes at a constant value after the predetermined equilibrium time T11. On the other hand, when there is a pressure leak, the absolute value of the differential pressure continues to increase without being a constant value as indicated by the broken line. In addition, when there is a minute pressure leak, it becomes an intermediate curve between these, as indicated by the alternate long and short dash line.

【0045】ここで、実施例3の圧力洩れ測定装置11
2では、所定の検出時間T9が経過した後でなければ、
これらの圧力洩れの大きさを求めることができなかっ
た。これに対して、本実施例の圧力洩れ測定装置202
では、零平衡直後の圧力が安定する過程において、差圧
センサ118からの出力電圧を演算処理部210で処理
して、差圧の単位時間当たりの変化量が算出される。こ
の差圧の変化率から、検出時間T12の経過後における
差圧の値が演算によって予測される。すなわち、圧力洩
れ測定装置202によれば、平衡段階において圧力洩れ
の有無と大きさを求めることができる。従って、検出時
間T12の経過を待つ必要がなく、測定時間を著しく短
縮することができる。なお、図9においては、圧力洩れ
のある場合とない場合の差を分かり易く示すために、平
衡段階(特に零平衡以降の段階)を拡大して図示してい
る。従って、図9の横軸に表される各段階の長さの比率
は、実際の測定時間の長さとは必ずしも対応していな
い。
Here, the pressure leak measuring device 11 according to the third embodiment is used.
In 2, unless the predetermined detection time T9 has elapsed,
It was not possible to determine the magnitude of these pressure leaks. On the other hand, the pressure leak measuring device 202 of the present embodiment
Then, in the process in which the pressure immediately after zero equilibrium stabilizes, the output voltage from the differential pressure sensor 118 is processed by the arithmetic processing unit 210 to calculate the amount of change in the differential pressure per unit time. From the rate of change of the differential pressure, the value of the differential pressure after the elapse of the detection time T12 is predicted by calculation. That is, according to the pressure leak measuring device 202, the presence or absence and the magnitude of the pressure leak can be obtained in the equilibrium stage. Therefore, it is not necessary to wait for the detection time T12 to elapse, and the measurement time can be significantly shortened. In FIG. 9, the equilibrium stage (particularly the stage after zero equilibrium) is shown in an enlarged manner in order to clearly show the difference between the case with pressure leak and the case without pressure leak. Therefore, the ratio of the lengths of the steps shown on the horizontal axis of FIG. 9 does not always correspond to the actual length of the measurement time.

【0046】なお演算処理部210には、ワーク温度に
よる影響とワーク容積による影響を補償する補償手段が
設けられている。例えばワークが極めて高温であると、
ワーク中に充填された気体がワークの熱によって加熱さ
れ、測定中にワーク中の気体圧力が増大する。一方密閉
配管部の温度は室温に等しく、圧力が温度によって影響
を受けることはない。このため、ワークからの気体洩れ
が実際にはなくとも、ワークの温度が極めて高温であれ
ばワーク側の圧力が高まって検出される差圧はプラス側
に増大する(図9中右上側に変化する)。この場合も、
ワーク側の圧力から密封配管側の圧力を減じた値を差圧
としており、前者が後者以上のときに差圧は正となる。
検出される差圧はリークによる変化(マイナス側への変
化)に加熱されることによる変化(プラス側への変化)
を加えたものとなる。そこでワーク温度補償手段は、ワ
ークの温度を入力し、それが高ければ検出された差圧を
マイナス側に修正して加熱による変化を相殺する。この
修正量はワーク温度が高いほど大きく修正される。
The arithmetic processing section 210 is provided with compensating means for compensating for the influence of the work temperature and the influence of the work volume. For example, if the workpiece is extremely hot,
The gas filled in the work is heated by the heat of the work, and the gas pressure in the work increases during the measurement. On the other hand, the temperature of the closed pipe section is equal to room temperature, and the pressure is not affected by the temperature. Therefore, even if there is no gas leakage from the workpiece, if the temperature of the workpiece is extremely high, the pressure on the workpiece side increases and the detected differential pressure increases to the plus side (changes to the upper right side in FIG. 9). To). Also in this case,
The value obtained by subtracting the pressure on the sealed piping side from the pressure on the work side is the differential pressure, and the differential pressure is positive when the former is the latter or higher.
Changes in the detected differential pressure due to heating (changes to the negative side) and changes due to heating (changes to the positive side)
Will be added. Therefore, the work temperature compensating means inputs the temperature of the work, and if it is high, corrects the detected differential pressure to the negative side to cancel the change due to heating. This correction amount is corrected more as the work temperature increases.

【0047】一方ワークの温度がさほど高くないと、気
体がワークに充填される際に気体が断熱圧縮されて昇温
され、それがワークによって冷やされる。このため測定
中に気体は冷却され、圧力が低くなってゆく。このとき
ワーク容積の方が密封配管の容積よりも大きいと、ワー
ク内の気体の方がすばやく冷却される。このために、ワ
ークからの気体洩れが実際にはなくとも、ワーク容積が
大で密封配管容積が小であると、ワーク側の圧力が低下
してマイナス側への差圧が発生する。この差圧は図9中
右下を向いたものとなる。そこで容積による補償手段
は、ワーク容積を入力し、それが大きければ、検出され
た差圧をプラス側に修正してリークによって生じる差圧
に対応するように補正する。このときの補正量はワーク
が大きいほど大きく修正される。ワーク温度とワーク容
積による補償は、実施例3の差圧自体を検出する方式に
も、実施例4の差圧の変化率を検出する方式にも適用さ
れる。
On the other hand, if the temperature of the work is not so high, when the work is filled with the gas, the gas is adiabatically compressed and heated, and the work is cooled. Therefore, the gas is cooled during the measurement, and the pressure becomes lower. At this time, if the work volume is larger than the sealed pipe volume, the gas in the work is cooled more quickly. For this reason, even if gas leakage from the work does not actually occur, if the work volume is large and the sealed pipe volume is small, the pressure on the work side decreases and a differential pressure to the negative side occurs. This differential pressure is directed to the lower right in FIG. Therefore, the volume-based compensating means inputs the work volume, and if it is large, corrects the detected differential pressure to the positive side and corrects it so as to correspond to the differential pressure caused by the leak. The correction amount at this time is corrected more as the work is larger. The compensation by the work temperature and the work volume is applied to both the method for detecting the differential pressure itself in the third embodiment and the method for detecting the rate of change of the differential pressure in the fourth embodiment.

【0048】[0048]

【発明の効果】請求項1に係る発明においては、配管の
一部を閉鎖することによって形成される密閉空間と被測
定物との差圧を検出することによって被測定物からの圧
力洩れを測定する圧力洩れ測定装置を創出したために、
測定用マスタを使用しない簡単な構成で差圧検出による
高精度の圧力洩れ測定を行うことができる。これによっ
て、低コストで高精度の圧力洩れ測定を行うことができ
る実用的な圧力洩れ測定装置となる。
According to the first aspect of the present invention, the pressure leak from the object to be measured is measured by detecting the differential pressure between the object to be measured and the closed space formed by closing a part of the pipe. To create a pressure leak measuring device that
It is possible to perform highly accurate pressure leak measurement by differential pressure detection with a simple configuration that does not use a measurement master. As a result, it becomes a practical pressure leak measuring device capable of performing highly accurate pressure leak measurement at low cost.

【0049】また、請求項2に係る発明においては、測
定用マスタを使用しない圧力洩れ測定装置を最小限の配
管構成で実現しているため、測定操作が簡単で装置の維
持管理も容易な圧力洩れ測定装置となる。これによっ
て、低い装置コスト及びランニングコストで高精度の圧
力洩れ測定が可能な実用的な圧力洩れ測定装置となる。
Further, in the invention according to claim 2, since the pressure leak measuring device which does not use the measuring master is realized with the minimum piping configuration, the pressure measuring operation is simple and the device maintenance is easy. It becomes a leak measuring device. As a result, it becomes a practical pressure leak measuring device capable of highly accurate pressure leak measurement with low device cost and running cost.

【0050】さらに、請求項3に係る発明においては、
被測定物に加圧気体を導入する第二の経路になるととも
に密閉空間と被測定物とを連通させる役割をする第三の
配管を追加した圧力洩れ測定装置を創出したために、被
測定物内の加圧が速まるとともに配管内の圧力がより均
一になる。これによって、短時間で精密な圧力洩れ測定
を行うことができる実用的な圧力洩れ測定装置となる。
Further, in the invention according to claim 3,
In order to create a pressure leak measuring device that adds a third pipe that serves as a second path for introducing pressurized gas to the measured object and also serves to connect the closed space and the measured object, As the pressurization of is accelerated, the pressure in the pipe becomes more uniform. As a result, it becomes a practical pressure leak measuring device capable of performing accurate pressure leak measurement in a short time.

【0051】また、請求項4に係る発明においては、加
圧気体源に対して被測定物の二次側に密閉空間となる配
管を接続した圧力洩れ測定装置を創出したために、被測
定物内と配管内の圧力が等しくなって高精度の測定が可
能になるとともに、短時間で測定することができる。こ
れによって、より短時間でより精密な圧力洩れ測定を行
うことができる、極めて実用的な圧力洩れ測定装置とな
る。
Further, in the invention according to claim 4, since the pressure leak measuring device in which the pipe serving as the closed space is connected to the secondary side of the object to be measured is connected to the pressurized gas source, the inside of the object to be measured is created. The pressures in the pipes are equalized, and highly accurate measurement is possible, and the measurement can be performed in a short time. As a result, it becomes a very practical pressure leak measuring device capable of performing more accurate pressure leak measurement in a shorter time.

【0052】さらに、請求項5に係る発明においては、
差圧の単位時間当たりの変化量から所定時間経過後の差
圧の大きさを予測する圧力洩れ測定方法を創出したため
に、圧力が安定する過程において測定結果を求めること
ができ、圧力が安定するまで待つ必要がない。これによ
って、測定時間を著しく短縮することができる、極めて
実用的な圧力洩れ測定方法となる。
Further, in the invention according to claim 5,
A pressure leak measurement method was created that predicts the magnitude of the differential pressure after a lapse of a predetermined time from the amount of change in the differential pressure per unit time, so the measurement result can be obtained in the process of stable pressure, and the pressure stabilizes. You don't have to wait until. As a result, it becomes a very practical pressure leak measuring method capable of significantly shortening the measuring time.

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

【図1】本発明に係る圧力洩れ測定装置及び圧力洩れ測
定方法の実施例1の基本的な構成及び操作を示す図であ
る。
FIG. 1 is a diagram showing a basic configuration and operation of a pressure leak measuring device and a pressure leak measuring method according to a first embodiment of the present invention.

【図2】圧力洩れ測定装置及び圧力洩れ測定方法の実施
例1の具体的な構成と測定の手順を示す図である。
FIG. 2 is a diagram showing a specific configuration and a measurement procedure of Example 1 of the pressure leak measuring device and the pressure leak measuring method.

【図3】圧力洩れ測定装置及び圧力洩れ測定方法の実施
例2の基本的な構成及び操作を示す図である。
FIG. 3 is a diagram showing a basic configuration and an operation of Example 2 of a pressure leak measuring device and a pressure leak measuring method.

【図4】圧力洩れ測定装置及び圧力洩れ測定方法の実施
例2の具体的な構成と測定の手順を示す図である。
FIG. 4 is a diagram showing a specific configuration and a measurement procedure of Example 2 of the pressure leak measuring device and the pressure leak measuring method.

【図5】圧力洩れ測定装置及び圧力洩れ測定方法の実施
例3の基本的な構成及び操作を示す図である。
FIG. 5 is a diagram showing the basic configuration and operation of Example 3 of the pressure leak measuring device and the pressure leak measuring method.

【図6】圧力洩れ測定装置及び圧力洩れ測定方法の実施
例3の具体的な構成と測定の手順を示す図である。
FIG. 6 is a diagram showing a specific configuration and a measurement procedure of Example 3 of the pressure leak measuring device and the pressure leak measuring method.

【図7】圧力洩れ測定装置及び圧力洩れ測定方法の実施
例3における測定結果を示す図である。
FIG. 7 is a diagram showing a measurement result in Example 3 of a pressure leak measuring device and a pressure leak measuring method.

【図8】圧力洩れ測定装置及び圧力洩れ測定方法の実施
例4の具体的な構成と測定の手順を示す図である。
FIG. 8 is a diagram showing a specific configuration and a measurement procedure of Example 4 of the pressure leak measuring device and the pressure leak measuring method.

【図9】圧力洩れ測定装置及び圧力洩れ測定方法の実施
例4における測定結果を示す図である。
FIG. 9 is a diagram showing a measurement result in Example 4 of the pressure leak measuring device and the pressure leak measuring method.

【符号の説明】[Explanation of symbols]

2,52,112,202 圧力洩れ測定装置 4,54,114 加圧気体源 8,58,118 差圧検出器 10A〜10E,60C〜60E 第一の配管 12A〜12C,62A,62B,64B,64A 第
二の配管 12B,62B,62C,64B,124B 独立した
密閉空間 14A 第一接続部 14B 第二接続部 20(30),70(80) 第二の開閉弁 40,90 第一の開閉弁 62C,62D 第三の配管 100 第三の開閉弁 120A,120B 一次側配管 122A 二次側配管 122B,124B,124A 閉ループ状配管 130 一次側開閉弁 140 閉ループ開閉弁 W 被測定物
2, 52, 112, 202 Pressure leak measuring device 4, 54, 114 Pressurized gas source 8, 58, 118 Differential pressure detector 10A to 10E, 60C to 60E First pipe 12A to 12C, 62A, 62B, 64B, 64A 2nd piping 12B, 62B, 62C, 64B, 124B Independent closed space 14A 1st connection part 14B 2nd connection part 20 (30), 70 (80) 2nd on-off valve 40, 90 1st on-off valve 62C, 62D Third piping 100 Third opening / closing valve 120A, 120B Primary side piping 122A Secondary side piping 122B, 124B, 124A Closed loop piping 130 Primary side opening / closing valve 140 Closed loop opening / closing valve W Measured object

Claims (5)

【特許請求の範囲】[Claims] 【請求項1】 加圧気体が導入された被測定物と独立し
た密閉空間との差圧を検出することによって前記被測定
物からの圧力洩れを測定する圧力洩れ測定装置であっ
て、 前記独立した密閉空間を前記圧力洩れ測定装置の配管の
一部を閉鎖することによって形成する圧力洩れ測定装
置。
1. A pressure leak measuring device for measuring a pressure leak from an object to be measured by detecting a differential pressure between the object to be measured into which a pressurized gas is introduced and an independent closed space, the pressure leakage measuring device comprising: A pressure leak measuring device, wherein the closed space is formed by closing a part of piping of the pressure leak measuring device.
【請求項2】 請求項1に記載された圧力洩れ測定装置
であって、 前記被測定物に加圧気体を導入するための加圧気体源を
前記被測定物と接続する第一の配管と、 その両端が各々前記加圧気体源に近い側の第一接続部と
前記被測定物に近い側の第二接続部において前記第一の
配管に接続された第二の配管と、 該第二の配管に設けられた差圧検出器と、 該差圧検出器と前記第一接続部との間において前記第二
の配管に設けられた第一の開閉弁と、 前記加圧気体源と前記第二接続部との間において前記第
一の配管に設けられた第二の開閉弁、とを有する圧力洩
れ測定装置。
2. The pressure leak measuring device according to claim 1, further comprising a first pipe connecting a pressurized gas source for introducing a pressurized gas to the object to be measured with the object to be measured. A second pipe whose both ends are respectively connected to the first pipe at a first connection part on the side close to the pressurized gas source and a second connection part on the side close to the object to be measured; A differential pressure detector provided in the pipe, a first opening / closing valve provided in the second pipe between the differential pressure detector and the first connecting portion, the pressurized gas source and the A pressure leak measuring device, comprising: a second opening / closing valve provided in the first pipe between the second connecting part and the second connecting part.
【請求項3】 請求項2に記載された圧力洩れ測定装置
であって、 その一端が前記第一の開閉弁と前記差圧検出器との間に
おいて前記第二の配管に接続され、他端が前記被測定物
に接続された第三の配管と、 該第三の配管に設けられた第三の開閉弁、とを有する圧
力洩れ測定装置。
3. The pressure leak measuring device according to claim 2, wherein one end is connected to the second pipe between the first on-off valve and the differential pressure detector, and the other end is connected. A pressure leak measuring device having a third pipe connected to the object to be measured, and a third opening / closing valve provided in the third pipe.
【請求項4】 加圧気体が導入された被測定物と独立し
た密閉空間との差圧を検出することによって前記被測定
物からの圧力洩れを測定する圧力洩れ測定装置であっ
て、 前記被測定物に加圧気体を導入するための加圧気体源を
前記被測定物と接続する一次側配管と、 該一次側配管に設けられた一次側開閉弁と、 前記被測定物に二次側配管を介して接続された閉ループ
状の配管と、 前記閉ループ状配管に設けられた差圧検出器及び閉ルー
プ開閉弁、とを有する圧力洩れ測定装置。
4. A pressure leak measuring device for measuring a pressure leak from an object to be measured by detecting a differential pressure between the object to be measured into which pressurized gas is introduced and an independent closed space, A primary side pipe that connects a pressurized gas source for introducing a pressurized gas to the measurement object with the measurement target object, a primary side opening / closing valve provided in the primary side piping, and a secondary side for the measurement target object A pressure leak measuring device comprising: a closed loop pipe connected via a pipe; and a differential pressure detector and a closed loop opening / closing valve provided in the closed loop pipe.
【請求項5】 被測定物に加圧気体を導入して、独立し
た密閉空間と前記被測定物との差圧を検出することによ
って前記被測定物からの圧力洩れを測定する圧力洩れ測
定方法であって、 前記差圧の単位時間当たりの変化量から所定時間経過後
の前記差圧の大きさを予測することによって前記被測定
物からの圧力洩れを測定する圧力洩れ測定方法。
5. A pressure leak measuring method for measuring pressure leak from an object to be measured by introducing a pressurized gas to the object to be measured and detecting a differential pressure between an independent closed space and the object to be measured. A pressure leak measuring method for measuring pressure leak from the object to be measured by predicting a magnitude of the differential pressure after a lapse of a predetermined time from a variation amount of the differential pressure per unit time.
JP15120494A 1994-07-01 1994-07-01 Pressure leak measuring device and pressure leak measuring method Expired - Lifetime JP3186438B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15120494A JP3186438B2 (en) 1994-07-01 1994-07-01 Pressure leak measuring device and pressure leak measuring method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15120494A JP3186438B2 (en) 1994-07-01 1994-07-01 Pressure leak measuring device and pressure leak measuring method

Publications (2)

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JPH0815079A true JPH0815079A (en) 1996-01-19
JP3186438B2 JP3186438B2 (en) 2001-07-11

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Country Status (1)

Country Link
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US7353692B2 (en) 2003-09-12 2008-04-08 Olympus Corporation Leakage tester
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US8502700B2 (en) 2007-11-29 2013-08-06 Airbus Operations Gmbh Apparatus and method for pressurising an aircraft cabin structure and measuring the amount of leakage of the aircraft cabin structure
JP2011504831A (en) * 2007-11-29 2011-02-17 エアバス・オペレーションズ・ゲーエムベーハー Apparatus and method for pressurizing an aircraft cabin structure and measuring the amount of leakage in the aircraft cabin structure
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CN113358292B (en) * 2020-03-03 2024-04-26 丰田自动车株式会社 Leak inspection device and leak inspection method

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