Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPH0812099B2 - Volume measuring device and its measuring method - Google Patents
[go: Go Back, main page]

JPH0812099B2 - Volume measuring device and its measuring method - Google Patents

Volume measuring device and its measuring method

Info

Publication number
JPH0812099B2
JPH0812099B2 JP62043914A JP4391487A JPH0812099B2 JP H0812099 B2 JPH0812099 B2 JP H0812099B2 JP 62043914 A JP62043914 A JP 62043914A JP 4391487 A JP4391487 A JP 4391487A JP H0812099 B2 JPH0812099 B2 JP H0812099B2
Authority
JP
Japan
Prior art keywords
volume
container
pressure
measured
differential pressure
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
JP62043914A
Other languages
Japanese (ja)
Other versions
JPS63208720A (en
Inventor
昭男 古瀬
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.)
Cosmo Instruments Co Ltd
Original Assignee
Cosmo Instruments Co Ltd
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 Cosmo Instruments Co Ltd filed Critical Cosmo Instruments Co Ltd
Priority to JP62043914A priority Critical patent/JPH0812099B2/en
Priority to US07/148,526 priority patent/US4888718A/en
Priority to KR1019880001587A priority patent/KR910004621B1/en
Publication of JPS63208720A publication Critical patent/JPS63208720A/en
Publication of JPH0812099B2 publication Critical patent/JPH0812099B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Landscapes

  • Measuring Volume Flow (AREA)

Description

【発明の詳細な説明】 「産業上の利用分野」 この発明は容器の内容席を測定するための装置と方法
に関する。
DETAILED DESCRIPTION OF THE INVENTION "Industrial application" The present invention relates to an apparatus and method for measuring the content seat of a container.

「従来技術」 従来容器の内容積を正確に測定する一方法として、例
えば流体、特に水を容器に入れ、容器が満たされるまで
に入れた水の量をもってその容器の内容積とする方法が
ある。
"Prior Art" Conventionally, as one method for accurately measuring the inner volume of a container, for example, there is a method in which a fluid, particularly water, is put in the container and the amount of water filled until the container is filled is used as the inner volume of the container. .

「発明が解決しようとする問題点」 生産工程で多数の容器の容積を水を使用して次々と測
定し、測定後に水を捨て、容器を乾燥させる必要がある
場合、使用した水の排水設備あるいは回収設備を必要と
し、又測定後の容器の乾燥設備も必要とされる。更に排
水、回収設備は水洩れが起らないよう対策を必要とす
る。このように水を使って容積測定を行うのは設備が大
きくなるし、乾燥のための設備と時間も余計に必要とさ
れる欠点がある。また水を扱うということはいろいろな
面でやっかいなものである。
"Problems to be solved by the invention" In the production process, the volume of a large number of containers is measured one after another using water, and after the measurement, it is necessary to discard the water and dry the containers. Alternatively, recovery equipment is required, and also equipment for drying the container after measurement is required. Furthermore, drainage and recovery facilities need measures to prevent water leakage. As described above, the volume measurement using water requires a large amount of equipment, and there is a drawback that equipment and time for drying are additionally required. Also, dealing with water is complicated in many ways.

水の代りに気体を使って同様の方法で容積測定を行う
ことを考えた場合、気体は圧縮性であるので容積測定は
その気体の圧力の影響を受け、かつ温度の影響も大き
い。また水と比べて気体は粘性が小さいことから容器自
体及び容器と測定装置の接続部等における気体の洩れが
大きく影響する。従って精度の高い測定は困難であっ
た。
Considering volumetric measurement in a similar manner using gas instead of water, the gas is compressible, so volumetric measurement is affected by the pressure of the gas and also by temperature. Further, since gas has a lower viscosity than water, leakage of gas in the container itself and the connection between the container and the measuring device has a great influence. Therefore, it is difficult to measure with high accuracy.

一方、特開昭54−84763号公報によれば、気体を使っ
た容積測定方法として、ボイル−シャルルの法則に基づ
き、被測定物に既知圧力、既知容積の容器を付加した場
合の圧力変化から被測定物の容積を測定することが記載
されている。しかしながら、この方法は圧力計によって
絶対圧力を測定するものであり、また基準容積となるも
のをもって、その容積を基準とした相対測定を行うもの
ではないため、測定誤差が生じやすく、よって例えば同
一仕様の多数の容器の容積のバラツキを測定する場合の
ように、高精度の測定を必要とする場合には適さないも
のであった。
On the other hand, according to JP-A-54-84763, as a volume measuring method using a gas, based on Boyle-Charles' law, a known pressure from a pressure change when a container of known volume is added to an object to be measured. It is described that the volume of an object to be measured is measured. However, this method measures absolute pressure with a pressure gauge, and does not perform relative measurement with the reference volume as the reference volume, so measurement errors are likely to occur, and therefore, for example, the same specifications It is not suitable when highly accurate measurement is required as in the case of measuring the variation in volume of a large number of containers.

この発明の目的は大きな設備と乾燥工程の必要を避け
るため、気体を使いかつ高い精度で容器の内容積を測定
することが可能であり、特に多数の容器の容積のバラツ
キを順次測定するのに適した容積測定装置と方法を提供
することである。
The object of the present invention is to avoid the need for a large facility and a drying process, so that it is possible to measure the internal volume of a container using gas and with high accuracy, and especially to measure the variation in the volume of a large number of containers sequentially. A suitable volume measuring device and method are provided.

「問題点を解決するための手段」 この発明によれば、被測定容器側と基準容器側のいず
れか一方に取付けられ、被測定容器側の容積と基準容器
側の容積とをほぼ均衡させる容積調整手段と、互いに等
しい容積とされ、互いに等しい圧力の気体が充填されて
被測定容器と基準容器とにそれぞれその気体を供給する
一対のタンクと、被測定容器側と基準容器側のいずれか
一方に既知の容積変化を与える手段と、被測定容器内の
圧力と基準容器内の圧力との差圧を測定する手段と、前
記容積変化を与えた場合と与えない場合の差圧の変化量
と、その与えた容積変化量とから検出感度を表す容積変
化に対する差圧変化の比を算出する手段と、差圧と検出
感度とから基準容器に対する被測定容器の容積差を算出
する手段とが設けられる。
[Means for Solving Problems] According to the present invention, a volume attached to either one of the measured container side and the reference container side, which substantially balances the measured container side volume and the reference container side volume. Adjusting means, a pair of tanks of equal volume and filled with gases of equal pressure to supply the gas to the measurement container and the reference container, respectively, either the measurement container side or the reference container side Means for giving a known volume change, means for measuring the differential pressure between the pressure in the container to be measured and the pressure in the reference container, and the amount of change in the differential pressure with and without the volume change. A means for calculating the ratio of the differential pressure change to the volume change representing the detection sensitivity from the given volume change amount, and a means for calculating the volume difference of the measured container with respect to the reference container from the differential pressure and the detection sensitivity. To be

更にこの発明による容積測定方法は、等しい圧力の気
体が充填された等しい容積を有する一対のタンクに感度
測定用容器及び基準容器をそれぞれ接続導通させ、その
導通後におけるそれら感度測定用容器内圧力と基準容器
内圧力との差圧を測定することをそれら感度測定用容器
と基準容器のいずれか一方に既知の容積変化を与えた場
合と与えない場合とについて行う工程と、その与えた容
積変化量と、測定した2つの差圧とから検出感度を表す
容積変化に対する差圧変化の比を算出する工程と、等し
い圧力の気体が充填さた前記一対のタンクに被測定容器
及び基準容器をそれぞれ接続導通させる工程と、その導
通後における被測定容器内圧力と基準容器内圧力との差
圧を測定する工程と、その測定した差圧と前記検出感度
とから基準容器に対する被測定容器の容積差を算出する
工程とを含む。
Further, the volume measuring method according to the present invention is such that the sensitivity measuring container and the reference container are connected to a pair of tanks having the same volume filled with gas of the same pressure, and the pressure is applied to the sensitivity measuring container after the conduction. The process of measuring the differential pressure from the reference container pressure with and without giving a known volume change to either one of the sensitivity measurement container and the reference container, and the given volume change amount. And a step of calculating the ratio of the differential pressure change to the volume change representing the detection sensitivity from the two measured differential pressures, and connecting the measured container and the reference container to the pair of tanks filled with gas of equal pressure. The step of conducting, the step of measuring the differential pressure between the pressure in the measured container and the reference internal pressure after the conduction, and the measurement of the differential pressure and the detection sensitivity to the reference container That includes a step of calculating the volume difference of the measured vessel.

「実施例」 機構部の構成 第1図はこの発明の実施例である容積測定装置の機構
部を示しており、以下の実施例の説明において容積測定
に使用する気体は空気である場合とする。
[Embodiment] Structure of mechanical part Fig. 1 shows a mechanical part of a volume measuring apparatus according to an embodiment of the present invention. In the following description of the embodiments, the gas used for volume measurement is air. .

圧縮空気源11の圧縮空気は配管により減圧弁12を介し
て二方電磁弁SV1とSV2の入口側に分岐して供給される。
二方電磁弁SV1とSV2の出口側にはそれぞれ等しい内容積
VMTのタンク13,14が配管で接続されている。タンク13,1
4はそれぞれ二方電磁弁SV3,SV4を介して測定側配管15と
基準側配管16に接続されている。測定側配管15及び基準
側配管16にはそれぞれ適当な治具を介して被測定容器17
と基準容器18が取り外し可能に取り付けられている。ま
た測定側配管15と基準側配管16との間にはそれら間の差
圧を測定するための差圧検出器19が配管により接続され
ている。更に測定側配管15と基準側配管16にはそれぞれ
排気用の二方電磁弁SV5,SV6が接続されている。減圧弁1
2の出口側にはタンク13,14に供給する空気圧の調節を目
視するための圧力計21が接続されている。また容積計算
に必要とされるデータとなるタンク13又は14内の圧力を
検出するための圧力検出器22がこの例ではタンク13に接
続されている。
The compressed air from the compressed air source 11 is branched and supplied to the inlet sides of the two-way solenoid valves SV 1 and SV 2 via a pressure reducing valve 12 by piping.
Two-way solenoid valves SV 1 and SV 2 have the same internal volume on the outlet side.
Tank 13, 14 VM T are connected by piping. Tank 13,1
4 is connected to the measurement side pipe 15 and the reference side pipe 16 via the two-way solenoid valves SV 3 and SV 4 , respectively. The measuring side pipe 15 and the reference side pipe 16 are respectively connected to the container to be measured 17 through an appropriate jig.
And a reference container 18 is removably attached. Further, a differential pressure detector 19 for measuring the differential pressure between the measurement side pipe 15 and the reference side pipe 16 is connected by a pipe. Further, two-way solenoid valves SV 5 and SV 6 for exhaust are connected to the measurement side pipe 15 and the reference side pipe 16, respectively. Pressure reducing valve 1
A pressure gauge 21 for visually checking the adjustment of the air pressure supplied to the tanks 13 and 14 is connected to the outlet side of 2. Further, a pressure detector 22 for detecting the pressure in the tank 13 or 14 which is data required for volume calculation is connected to the tank 13 in this example.

タンク13と、被測定容器17と、これらに接続された配
管部分とを含む互いに気体が導通された閉じた系を測定
側空気系と呼ぶ。同様にタンク14と、基準容器18と、こ
れらに接続された配管部分とを含む互いに気体が導通さ
れた閉じた系を基準側空気系と呼ぶ。測定側配管15には
既知の容積変化を測定側空気系に与えるための容積付加
器23が接続されており、基準側配管16には測定側空気系
の全容積と基準側空気系の全容積とのバランスを調整す
るための容積調整器24が接続されている。容積付加器23
は例えばシリンダとその中で移動可能なピストンで構成
され、ピストンの移動可能な長さをあらかじめ設定する
ことができ、この例では三方電磁弁SV7を介して圧縮空
気によりピストンを駆動する。容積調整器24もシリンダ
とピストンより構成され、つまみ24−1を回動すること
によりピストンを移動することができる。
A closed system, which includes the tank 13, the container 17 to be measured, and a pipe portion connected to the tank 13 and through which gas is conducted, is called a measurement side air system. Similarly, a closed system including the tank 14, the reference container 18, and a pipe portion connected to the tank 14 and in which gas is conducted is called a reference side air system. The measurement side pipe 15 is connected with a volume adder 23 for giving a known volume change to the measurement side air system, and the reference side pipe 16 is the total volume of the measurement side air system and the reference side air system. A volume adjuster 24 for adjusting the balance with Volume adder 23
Is composed of, for example, a cylinder and a piston movable therein, and the movable length of the piston can be preset. In this example, the piston is driven by compressed air via a three-way solenoid valve SV 7 . The volume adjuster 24 is also composed of a cylinder and a piston, and the piston can be moved by rotating the knob 24-1.

原 理 上述の構成において測定側空気系と基準側空気系が大
気圧に放置された状態で電磁弁SV3,SV4,SV5,SV6を閉じ
る。次に電磁弁SV1,SV2を開きタンク13,14に圧力PTの空
気を充填し、その後に電磁弁SV1,SV2を閉じ電磁弁SV3,S
V4を開けた場合に差圧検出器19で検出される差圧ΔPが
どのように表わされるかを検出する。
In the above configuration, the solenoid valves SV 3 , SV 4 , SV 5 and SV 6 are closed while the measurement side air system and the reference side air system are left at atmospheric pressure. Next, the solenoid valves SV 1 and SV 2 are opened and the tanks 13 and 14 are filled with air at the pressure P T , and then the solenoid valves SV 1 and SV 2 are closed and the solenoid valves SV 3 and SV 2 are closed.
It is detected how the differential pressure ΔP detected by the differential pressure detector 19 when V 4 is opened is represented.

タンク13,14の配管部をも含む容積は互いに等しく
VT、被測定容器17とそれに接続された測定側配管15を含
む容積をVW、基準容器18とそれに接続された基準側配管
16を含む容積をVM、電磁弁SV3,SV4を開けた後の測定側
及び基準側空気系の圧力をそれぞれPW,PM、差圧検出器
で検出される差圧をΔPとする。
The volumes including the piping of tanks 13 and 14 are equal to each other.
V T , the volume containing the container 17 to be measured and the measurement side pipe 15 connected to it V W , the reference container 18 and the reference side pipe connected to it
The volume including 16 is V M , the pressures of the measurement side and reference side air systems after opening the solenoid valves SV 3 and SV 4 are P W and P M , respectively, and the differential pressure detected by the differential pressure detector is ΔP. To do.

VW−VM=ΔV ……(1) PW−PM=ΔP ……(2) ボイルの法則より次式が成立する。V W −V M = ΔV (1) P W −P M = ΔP (2) From Boyle's law, the following formula is established.

VT・PT=(VT+VM)・PM ……(3) VT・PT=(VT+VW)・PW ……(4) 式(1),(2)を式(4)に代入し、その結果に式
(3)のPMを代入すると、 となり、これによりΔPは次式で表わされる。
V T · P T = (V T + V M ) · P M …… (3) V T · P T = (V T + V W ) · P W …… (4) Formulas (1) and (2) Substituting into (4) and substituting P M in equation (3) into the result, Therefore, ΔP is expressed by the following equation.

ここでΔV≪(VT+VM)が成り立つとすると式(5)は
次のように近似できる。
Assuming that ΔV << (V T + V M ) holds, the equation (5) can be approximated as follows.

式(6)から次の事が理解できる。即ち、第1図に示
す構成においてVT,VMは変化しないとみなせるので、測
定側空気系と基準側空気系との容積差ΔVがある場合、
電磁弁SV3,SV4を開けた後に検出される差圧ΔPはタン
ク13,14に与えた初期圧力PTと容積差ΔVの積に比例す
る。その比例定数KはK=VT/(VT+VMであり、ΔP
/ΔV=Sとおけば式(6)は次のように変形できる。
The following can be understood from the equation (6). That is, since it can be considered that V T and V M do not change in the configuration shown in FIG. 1, when there is a volume difference ΔV between the measurement side air system and the reference side air system,
The differential pressure ΔP detected after opening the solenoid valves SV 3 and SV 4 is proportional to the product of the initial pressure P T applied to the tanks 13 and 14 and the volume difference ΔV. The proportional constant K is K = V T / (V T + V M ) 2 , and ΔP
If / ΔV = S, then equation (6) can be transformed as follows.

Sは第1図の構成における差圧検出器19の容積差に対
する差圧検出感度を表わしている。
S represents the differential pressure detection sensitivity with respect to the volume difference of the differential pressure detector 19 in the configuration of FIG.

タンク13,14に与える初期圧力PTが一定であれば式
(7)はΔVが充分小さい範囲では常に成立するといえ
るので異なる容積差ΔV1,ΔV2に対しそれぞれS=ΔP1/
ΔV1,S=ΔP2/ΔV2であれば次式が成立する。
If the initial pressure P T given to the tanks 13 and 14 is constant, it can be said that the equation (7) is always satisfied in the range where ΔV is sufficiently small. Therefore, for different volume differences ΔV 1 and ΔV 2 , S = ΔP 1 /
If ΔV 1 and S = ΔP 2 / ΔV 2 , the following equation holds.

即ち、異なる容積差ΔV1,ΔV2を与える2つの被測定
容器を接続した場合についてそれぞれ差圧ΔP1,ΔP2
測定し、式(8)により感度Sを計算することができ
る。実際には1つの被測定容器についてまず差圧ΔP1
測定し、次に両空気系を大気開放した後に容積付加器23
により既知の容積ΔVsを付加し、同様に差圧ΔP2を測定
する。付加した容積ΔVsは式(8)における容積差の変
化分(ΔV2−ΔV1)であり、従って式(8)から感度S
が計算できる。
That is, the differential pressures ΔP 1 and ΔP 2 are respectively measured in the case where two containers to be measured which give different volume differences ΔV 1 and ΔV 2 are connected, and the sensitivity S can be calculated by the equation (8). Actually, first, the differential pressure ΔP 1 is measured for one container to be measured, and then both air systems are opened to the atmosphere, and then the volume adder 23
A known volume ΔV s is added by and the differential pressure ΔP 2 is similarly measured. The added volume ΔV s is the variation (ΔV 2 −ΔV 1 ) of the volume difference in the equation (8), and therefore the sensitivity S is calculated from the equation (8).
Can be calculated.

測定側空気系と基準側空気系の配管の内容積が同じに
なるよう設計すれば式(1)においてΔVは被測定容器
17と基準容器18との容積差に等しい。従ってあらかじめ
決めた初期圧力PTに対し上述のように感度Sが計算され
ると、この感度Sを使って未知の容積を持つ他の被測定
容器17と基準容器18との容積差ΔVを次式で求めること
ができる。
If it is designed so that the inner volumes of the piping of the measurement side air system and the reference side air system are the same, ΔV in equation (1) is
Equal to the volume difference between 17 and the reference container 18. Therefore, when the sensitivity S is calculated as described above with respect to a predetermined initial pressure P T , the sensitivity S is used to calculate the volume difference ΔV between another measured container 17 having an unknown volume and the reference container 18 as follows. It can be obtained by a formula.

ΔV=ΔP/S ……(9) 被測定容器17と基準容器18の容積をそれぞれVXw,Vm
表わせば被測定容器17の容積Vwは Vw=vm+ΔV ……(10) で計算できる。但し、測定精度を挙げるためにはΔV≪
(VT+VM)の条件を充分満足させる必要があり、そのた
めには容積差ΔV自身が小さいことが好ましい。即ち、
基準容器18としては被測定容器17の容積とできるだけ近
いものを選択することが望ましい。生産された同一種類
の多数の容積のバラツキを測定するのであれば、それら
の容器の適当なものを1つ選んでそれを基準容器18とし
て使用し、式(9)によりその基準容器18に対する他の
容器の容積差を次々と測定することが可能となる。
ΔV = ΔP / S (9) If the volumes of the measuring container 17 and the reference container 18 are expressed as VX w and V m , the volume V w of the measuring container 17 is V w = v m + ΔV (10) Can be calculated by However, to increase the measurement accuracy, ΔV <<
It is necessary to sufficiently satisfy the condition of (V T + V M ), and for that purpose, it is preferable that the volume difference ΔV itself is small. That is,
As the reference container 18, it is desirable to select a container as close as possible to the volume of the container 17 to be measured. If you want to measure the variation of a large number of volumes of the same type produced, select an appropriate one of these containers and use it as the reference container 18, and use the formula (9) It is possible to successively measure the volume difference between the containers.

一般的には設計された各種の被測定容器の設計容器は
あらかじめわかっているので接続する被測定容器の種類
を変える場合に基準容器19を変更するかわりに容積調整
器24により所望の基準容積とほぼ同じとなるよう調整設
定してもよい。この調整によりΔvの容積が基準容器18
に与えられ、被測定容器17の容積とほぼ同じ容積の基準
容器を装着したことと等価になる。容積調整器24による
調整の後に前述のように差圧ΔP1,ΔP2を測定し、式
(8)から感度を計算する。この場合、以後の容積測定
において基準容器18の内容積は(Vm+Δv)であるとみ
なして式(10)の計算を行う。即ち Vw=Vm+Δv+ΔV ……(11) によって被測定容器17の容積を計算する。
Generally, the designed container of various designed measured containers is known in advance, so that instead of changing the reference container 19 when changing the type of the measured container to be connected, a desired reference volume is obtained by the volume adjuster 24. You may adjust and set so that it may become substantially the same. By this adjustment, the volume of Δv can be adjusted to the standard container 18
And is equivalent to mounting a reference container having substantially the same volume as the volume of the measured container 17. After the adjustment by the volume adjuster 24, the differential pressures ΔP 1 and ΔP 2 are measured as described above, and the sensitivity is calculated from the equation (8). In this case, in the subsequent volume measurement, the internal volume of the reference container 18 is considered to be (V m + Δv), and the calculation of the equation (10) is performed. That is, the volume of the container 17 to be measured is calculated by V w = V m + Δv + ΔV (11).

差圧補正 上述においては被測定容器17は洩れの無いものとして
考えてきたが、次に微少な洩れがあった場合について検
討する。もし洩れが無ければ電磁弁SV3,SV4を時点t0
開けた後の測定側及び基準側空気系間の差圧は第3図の
一点鎖線(イ)で示すように短時間δのうちに一定値に
達し、その後変化はしない。これを差圧検出器19で観測
した場合は、差圧検出器として例えばダイアフラム型差
圧検出器を使用した場合はそのダイアフラムの変位の応
答が遅いこととその過渡現象のため実線(ロ)で示すよ
うに立上りが遅くかつオーバーシュートした後に前記一
定値に戻る。所が、被測定容器17にその内容積に比べて
微少な洩れがある場合は時間とともに測定側空気系の圧
力が減少し、従って差圧検出器19の出力も変化する。こ
の変化は短い時間内では直線的変化とみなせるので、差
圧検出器19の応答特性も考慮すると検出された差圧は実
線(ハ)に示すように変化する。電磁弁SV3,SV4を開け
た直後(例えばδ後)においては実線に洩れて出た空気
の量は無視できる程少いのでその時の差圧を正しい差圧
として使えばよい。その差圧は実線(ハ)の直線部分を
延長して時点t0における縦軸(差圧)と交叉する点の差
圧値ΔP0とほぼ等しい。実線(ハ)の直線領域内におけ
る時点t1とt2とで検出した差圧をΔP1,ΔP2とするとΔP
0は次式で与えられる。
Differential Pressure Correction In the above description, it has been considered that the container 17 to be measured has no leak, but next, a case where a slight leak occurs will be examined. If there is no leakage, the differential pressure between the measurement side and reference side air systems after opening solenoid valves SV 3 and SV 4 at time t 0 is δ for a short time as shown by the one-dot chain line (a) in FIG. It reaches a certain value in a while and does not change thereafter. When this is observed by the differential pressure detector 19, for example, when a diaphragm type differential pressure detector is used as the differential pressure detector, the response of the displacement of the diaphragm is slow and the transient phenomenon shows the solid line (b). As shown, the rising speed is slow and after the overshoot, it returns to the constant value. However, when there is a slight leak in the container 17 to be measured compared to its internal volume, the pressure in the measurement side air system decreases with time, and the output of the differential pressure detector 19 also changes. Since this change can be regarded as a linear change within a short time, the differential pressure detected changes as shown by the solid line (c) when the response characteristic of the differential pressure detector 19 is also taken into consideration. Immediately after opening the solenoid valves SV 3 and SV 4 (for example, after δ), the amount of air leaking to the solid line is so small that it can be ignored, so the differential pressure at that time may be used as the correct differential pressure. The differential pressure is substantially equal to the differential pressure value ΔP 0 at the point where the straight line portion of the solid line (C) is extended and the vertical axis (differential pressure) intersects at time t 0 . Let ΔP 1 and ΔP 2 be the pressure differences detected at time points t 1 and t 2 in the straight line area of the solid line (c)
0 is given by the following equation.

式(12)により求めた差圧ΔP0を式(9)のΔPの代
りに使えば被測定容器17に洩れがあっても高い精度で基
準容器18に対する容積差ΔVを求めることができる。式
(12)は洩れに対する差圧の補正を表わしているが、洩
れ以外の原因、例えば閉じた空気系内の気体の温度低下
によっても差圧に変化が生じる。しかしながらその変化
が短期間内で直線的であるとみなせるならば、同様に補
正が可能である。結局式(12)による補正は、洩れ、温
度変化、その他すべての原因による総合的な差圧変化を
補正していることになる。
If the differential pressure ΔP 0 obtained by the equation (12) is used instead of ΔP in the equation (9), the volume difference ΔV with respect to the reference container 18 can be obtained with high accuracy even if the measured container 17 leaks. Equation (12) represents the correction of the differential pressure with respect to the leak, but the differential pressure also changes due to causes other than the leak, for example, the temperature decrease of the gas in the closed air system. However, if the change can be considered to be linear within a short period of time, correction is possible as well. After all, the correction by the equation (12) corrects the total differential pressure change due to leakage, temperature change, and all other causes.

感度補正 同じ値の検出感度Sを使って式(9)により多数の容
器の基準容器18に対する容積差ΔVを順次測定していく
場合、式(7)から明らかなようにタンク13,14に与え
る初期圧力PTは測定毎に常に同じである必要があるが、
圧縮空気源11の圧力が変化すれば当然PTも変化する。し
かしながらタンク13,14の容積VT及び基準容積18の容積V
Mは変化しないので比例定数 K=VT/(VT+VMは一定である。従ってタンク13,14
に与える初期圧力がP′の時の検出感度をS′と表わ
せば次式が成立する。
Sensitivity correction When the volume differences ΔV of a large number of containers with respect to the reference container 18 are sequentially measured by the formula (9) using the detection sensitivity S of the same value, they are given to the tanks 13 and 14 as apparent from the formula (7) The initial pressure P T should always be the same from measurement to measurement,
If the pressure of the compressed air source 11 changes, naturally P T also changes. However, the volumes V T of the tanks 13 and 14 and the volume V T of the reference volume 18
Since M does not change, the proportionality constant K = V T / (V T + V M ) 2 is constant. Therefore tanks 13,14
Initial pressure following equation holds Expressed as 'S detection sensitivity when the T' P applied to the.

S′=−K・P′ ……(13) 式(7)と(13)により次式が得られる。S ′ = − K · P ′ T (13) The following equation is obtained from the equations (7) and (13).

S′=S・P′T/PT ……(14) 従って各被測定器17の測定において電磁弁SV1,SV2
開けてタンク13,414に充填した空気の圧力P′を圧力
検出器22により検出し、式(14)により感度を補正し、
その補正した感度S′を式(9)における感度Sの代り
に使えばよく、容積測定毎にあらかじめ容積付加器23を
駆動して感度測定を行う必要はない。
S ′ = S · P ′ T / P T (14) Therefore, in the measurement of each device under test 17, the solenoid valves SV 1 and SV 2 are opened and the pressure P ′ T of the air filled in the tanks 13,414 is detected by the pressure detector. Detected by 22 and corrected the sensitivity by equation (14),
The corrected sensitivity S'may be used instead of the sensitivity S in the equation (9), and it is not necessary to drive the volume adder 23 in advance for each volume measurement to perform the sensitivity measurement.

制御部の構成 第2図は第1図の容積測定機構部の動作を制御し、か
つ各種定数及び測定値を受けて検出感度Sあるいは容積
差ΔV等を計算するための制御部を示し、マイクロコン
ピュータ31とその他の周辺回路とから構成されている。
マイクロコンピュータ31はCPU41,RAM42,ROM43、入力ポ
ート44、出力ポート45を含み、これらは共通バス46を介
して互いに接続されている。
Structure of Control Unit FIG. 2 shows a control unit for controlling the operation of the volume measuring mechanism unit shown in FIG. 1 and for calculating the detection sensitivity S or the volume difference ΔV etc. by receiving various constants and measured values. It is composed of a computer 31 and other peripheral circuits.
The microcomputer 31 includes a CPU 41, a RAM 42, a ROM 43, an input port 44 and an output port 45, which are connected to each other via a common bus 46.

第1図における差圧検出器19及び圧力検出器22の出力
はマルチプレクサ32の入力側にそれぞれ接続され、差圧
信号ΔP及び圧力信号PTの一方が選択されて出力側に接
続される。マルチプレクサ32の出力側は増幅器33に接続
され、差圧信号ΔP又は圧力信号PTが増幅される。増幅
器33の出力はAD変換器の入力に接続されディジタル信号
に変換されるとともにモニター用のメータ35にも接続さ
れアナログ表示される。AD変換器34の出力は入力ポート
44を介してコンピュータ31内に取込まれる。入力ポート
44には各種タイマの設定時間T1,T2,T3及び容積付加器23
に設定する付加容積ΔVを入力するためのキーボード36
が接続されている。出力ポート45には計算結果を表示す
るための表示器37、及び第1図における各電磁弁の開閉
駆動を行うための駆動回路38が接続されている。ROM43
にはこの発明の装置による検出感度測定と容積差測定の
ための第4図及び第5図に示す動作手順がプログラムと
して記憶されており、CPUはこのプログラムに従って駆
動回路38による電磁弁SV1〜SV7の開閉制御、マルチプレ
クサ32における信号の選択、表示器37における計算結果
の表示、指示器39に対する指示表示等の他に検出感度、
及び測定容積等の必要な計算を実行する。
The outputs of the differential pressure detector 19 and the pressure detector 22 in FIG. 1 are respectively connected to the input side of the multiplexer 32, and one of the differential pressure signal ΔP and the pressure signal P T is selected and connected to the output side. The output side of the multiplexer 32 is connected to the amplifier 33, and the differential pressure signal ΔP or the pressure signal P T is amplified. The output of the amplifier 33 is connected to the input of the AD converter to be converted into a digital signal, and is also connected to the monitor meter 35 for analog display. Output of AD converter 34 is an input port
Captured into computer 31 via 44. Input port
44 are set times T 1 , T 2 , T 3 of various timers and a volume adder 23
Keyboard for inputting additional volume ΔV to be set in
Is connected. The output port 45 is connected to a display 37 for displaying the calculation result and a drive circuit 38 for opening / closing the solenoid valves in FIG. ROM43
The operating procedure shown in FIGS. 4 and 5 for measuring the detection sensitivity and measuring the volume difference by the device of the present invention is stored as a program, and the CPU operates the solenoid valves SV 1 to SV 1 through the drive circuit 38 in accordance with the program. SV 7 opening and closing control, selection of signals in the multiplexer 32, display of calculation results on the display 37, detection sensitivity in addition to indication display for the indicator 39,
And perform necessary calculations such as measuring volume.

動 作(感度測定) この発明では前述したように、差圧検出器19を使用し
て、その測定した差圧ΔPから被測定容器17と基準容器
18との容積差ΔVを求めるものであり、容積測定を行う
前に、まず差圧検出器19の容積差ΔVに対する検出感度
Sを測定する。そのためには洩れのない被測定容器17を
感度測定用容器として測定側配管15に接続する。次に容
積付加器23により与えるあらかじめ決めた付加容積Δ
Vs、即ちピストンの移動可能距離を設定する。更に圧力
計21の指示を監視しながら減圧弁12を調節してタンク1
3,14に与える空気の圧力を設定する。設定が終ると操作
者はキーボード36により開始の指示を入力する。以下第
4図に示す動作のフローチャートに従って第1図の機構
部を制御しかつ第2図の制御部で測定データにもとづき
各種計算を行う。
Operation (sensitivity measurement) As described above, in the present invention, the differential pressure detector 19 is used to measure the measured differential pressure ΔP from the measured container 17 and the reference container.
The volume difference ΔV with respect to 18 is obtained. Before the volume measurement, the detection sensitivity S for the volume difference ΔV of the differential pressure detector 19 is measured. For that purpose, a leak-proof container 17 to be measured is connected to the measurement side pipe 15 as a sensitivity measuring container. Next, a predetermined additional volume Δ given by the volume adder 23
Set V s , that is, the movable distance of the piston. Further, while monitoring the instruction of the pressure gauge 21, the pressure reducing valve 12 is adjusted and the tank 1
Set the pressure of the air given to 3,14. When the setting is completed, the operator inputs a start instruction using the keyboard 36. The mechanical section of FIG. 1 is controlled according to the flow chart of the operation shown in FIG. 4 and various calculations are performed by the control section of FIG. 2 based on the measurement data.

ステップS1で電磁弁SV3,SV4,SV7を閉じ、SV5,SV6を開
き大気に開放する。ステップS2で電磁弁SV1,SV2を開け
タンク13,14に設定した圧力の空気を充填する。ステッ
プS3でRAM42内の所定のアドレスに設定したT1タイマを
始動し、時間T1が経過したかを判定する。T1が経過した
ならばタンク13,14内の圧力は平衡に達したと判断して
ステップS4で電磁弁SV1,SV2,SV5,SV6閉じ、ステップS5
で電磁弁SV3,SV4を開く。ステップS6でRAM42の所定のア
ドレスに設定したT2タイマを始動し、時間T2が経過した
かを判定する。T2が経過したならば測定側空気系及び基
準側空気系の圧力はそれぞれ平衡に達っしたと判断しス
テップS7でマルチプレクサ32により差圧ΔPを選択して
差圧検出器19からその時の検出差圧ΔP1を取込みRAM42
の所定アドレスに記憶する。ステップS8で電磁弁SV3,SV
4を閉じ、SV5,SV6をベントして測定側及び基準側空気系
を大気圧に開放する。ステップS9でRAM42の所定アドレ
スに設定したT3タイマを始動し、時間T3が経過したかを
判定する。T3が経過したならばステップS10で電磁弁SV7
を導通させて、容積付加器23のピストンを駆動し、あら
かじめ設定した可動距離だけ移動させて所定の容積ΔVs
を測定側空気系に付加する。ステップS11で再び電磁弁S
V1,SV2を開きタンク13,14内を設定圧力に加圧する。ス
テップS12でT1タイマを始動し、時間T1が経過したかを
判定する。T1が経過したならばステップS13でマルチプ
レクサ32によりタンク圧PTを選択して圧力検出器22から
その時の検出タンク圧PTを取込みRAM42の所定アドレス
に記憶する。ステップS14で電磁弁SV1,SV2,SV5,SV6を閉
じ、ステップS15で電磁弁SV3,SV4を開く。ステップS16
でT2タイマを再び始動させ時間T2が経過したかを判定す
る。T2が経過したならばステップS17でマルチプレクサ3
2により差圧ΔPを選択して差圧検出器19からの検出差
圧ΔP2を取込みRAM42の所定アドレスに記憶する。ステ
ップS18で差圧ΔP1とΔP2の差ΔP′を計算し、ステッ
プS19で付加した容積ΔVsと差圧変化量ΔP′とから検
出感度Sを計算する。次にステップS20で電磁弁SV3,SV4
を閉じ、電磁弁SV5,SV6を開き、空気系を大気に開放
(ベント)し電磁弁SV7をベントする。次にステップS21
で再びT3タイマを始動し、時間T3が経過したならばステ
ップS22で指示器39を点灯して感度測定を終了する。ス
テップS19で計算された感度SはRAM42の所定アドレスに
記憶しておく。
Close the solenoid valve SV 3, SV 4, SV 7 in step S 1, is open to the atmosphere opens the SV 5, SV 6. At step S 2 , the solenoid valves SV 1 and SV 2 are opened and the tanks 13 and 14 are filled with air having the set pressure. In step S 3 , the T 1 timer set at a predetermined address in the RAM 42 is started and it is determined whether the time T 1 has elapsed. If T 1 is passed the pressure in the tank 13, 14 solenoid valves SV 1, SV 2, SV 5 , SV 6 closed in step S 4 is judged to have reached the equilibrium, Step S 5
Open solenoid valves SV 3 and SV 4 with. In step S 6 , the T 2 timer set in the predetermined address of the RAM 42 is started and it is determined whether the time T 2 has elapsed. When T 2 has elapsed, it is determined that the pressures of the measurement side air system and the reference side air system have reached equilibrium, and in step S 7 , the differential pressure ΔP is selected by the multiplexer 32 to select the differential pressure detector 19 from the differential pressure detector 19 at that time. Incorporate detection differential pressure ΔP 1 RAM 42
Is stored at a predetermined address of. Solenoid valves SV 3 , SV in step S 8
4 is closed and SV 5 and SV 6 are vented to open the measurement side and reference side air systems to atmospheric pressure. Start the T 3 timer set to a predetermined address in RAM42 in step S 9, determines whether elapsed time T 3. Solenoid valve SV 7 in step S 10 if T 3 has elapsed
To drive the piston of the volumetric adder 23 and move it by a preset movable distance to obtain a predetermined volume ΔV s.
Is added to the measurement side air system. Solenoid valve S again in step S 11
Open V 1 and SV 2 and pressurize the tanks 13 and 14 to the set pressure. In step S 12 , the T 1 timer is started and it is determined whether the time T 1 has elapsed. When T 1 has elapsed, the tank pressure P T is selected by the multiplexer 32 in step S 13 and the detected tank pressure P T at that time is fetched from the pressure detector 22 and stored in a predetermined address of the RAM 42. Close the solenoid valve SV 1, SV 2, SV 5 , SV 6 at step S 14, opening the solenoid valve SV 3, SV 4 in step S 15. Step S 16
Then, restart the T 2 timer and determine whether the time T 2 has elapsed. If T 2 has elapsed, then in step S 17 the multiplexer 3
The differential pressure ΔP is selected by 2 and the detected differential pressure ΔP 2 from the differential pressure detector 19 is fetched and stored in a predetermined address of the RAM 42. In step S 18 , the difference ΔP ′ between the differential pressures ΔP 1 and ΔP 2 is calculated, and in step S 19 , the detection sensitivity S is calculated from the added volume ΔV s and the differential pressure change amount ΔP ′. Then the solenoid valve SV 3 in step S 20, SV 4
Is closed, solenoid valves SV 5 and SV 6 are opened, the air system is opened (vented) to the atmosphere, and solenoid valve SV 7 is vented. Then step S 21
Then, the T 3 timer is started again, and if the time T 3 has elapsed, the indicator 39 is turned on in step S 22 to end the sensitivity measurement. The sensitivity S calculated in step S 19 is stored in the RAM 42 at a predetermined address.

動 作(容積測定) 次に第5図に示すフローチャートに従って被測定容器
17と基準容器18の容積差ΔV及び被測定容器17の内容積
Vwを測定する動作について説明する。
Operation (volume measurement) Next, according to the flow chart shown in FIG.
Volume difference ΔV between reference container 17 and reference container 18 and internal volume of container 17 to be measured
The operation of measuring V w will be described.

被測定容器17を測定側配管15に取付けた後、操作者が
キーボードより開始の指示を行うとステップS1で電磁弁
SV3,SV4を閉じ、SV5,SV6を開く。ステップS2で電磁弁SV
1,SV2を開き、タンク13,14に設定された圧力の空気を充
填する。ステップS3でRAM42内の所定アドレスに設定し
たT1タイマを始動させ、時間T1が経過したかを判定す
る。T1が経過したならばステップS4でタンク内圧力P′
を測定する。ステップS5で感度測定工程においてRAM4
2に記憶したタンク圧力PTと感度Sを読み出し補正感度
S′を式(14)により計算する。ステップS6で電磁弁SV
1,SV2,SV5,SV6を閉じ、ステップS7で電磁弁SV3,SV4を開
く。次にステップS8でRAM42の所定のアドレスに設定し
たT2タイマを始動し、時間T2が経過したかを判定する。
T2が経過したならばステップS9で測定側と基準側の空気
系の圧力差ΔP1を測定RAM42に取込む。ステップS10でRA
M42の所定アドレスに設定したT4タイマを始動し時間T4
が経過したかを判定する。T4が経過したならばステップ
S11で再び2つの空気系の差圧ΔP2を測定しRAM42に取込
む。ステップ12でRAM42から測定差圧ΔP1,ΔP2及びタイ
マ時間T2,T4、即ち第3図における(t1−t0)および(t
2−t1)を読み出し、式(12)により補正差圧ΔP0を計
算する。ステップS13でRAM42から補正感度S′を読み出
し式(9)により基準容器18に対する被測定容器17の補
正された容積差ΔVを計算する。次にステップS14で容
積差ΔVを表示器37に表示し、ステップS15で電磁弁S
V3,SV4を閉じ、電磁弁SV5,SV6を開く。ステップS16でT3
タイマを始動し、時間T3が経過したならばステップS17
で指示器39を転倒し測定を終了する。もし必要であれば
ステップS13とS14の間で被測定容器17の容積Vwを式(1
0)により計算するステップS′13を点線で示すように
設けてもよい。
After mounting the container to be measured 17 in the measurement pipe 15, when the operator performs an instruction to start the keyboard solenoid valve in step S 1
Close SV 3 and SV 4 and open SV 5 and SV 6 . Solenoid valve SV in step S 2
1 , SV 2 is opened, and the tanks 13 and 14 are filled with the air having the set pressure. In step S 3 , the T 1 timer set in the RAM 42 at a predetermined address is started to determine whether the time T 1 has elapsed. If T 1 has elapsed, in step S 4 the tank pressure P ′
Measure T. In Step S 5 in sensitivity measuring step RAM4
The tank pressure P T and the sensitivity S stored in 2 are read out, and the corrected sensitivity S ′ is calculated by the equation (14). Solenoid valve SV in step S 6
1 , SV 2 , SV 5 and SV 6 are closed, and solenoid valves SV 3 and SV 4 are opened in step S 7 . Then start the T 2 timer set to a predetermined address in RAM42 in step S 8, determines whether the elapsed time T 2.
When T 2 has elapsed, the pressure difference ΔP 1 between the measurement side and the reference side air system is taken into the measurement RAM 42 in step S 9 . RA in the step S 10
Start of T 4 timer set to a predetermined address of the M42 time T 4
Is determined. Step if T 4 has passed
At S 11 , the differential pressure ΔP 2 between the two air systems is measured again and taken into RAM 42. In step 12 , the measured differential pressures ΔP 1 and ΔP 2 and the timer times T 2 and T 4 are read from the RAM 42, that is, (t 1 −t 0 ) and (t
2− t 1 ) is read and the corrected differential pressure ΔP 0 is calculated by the equation (12). In step S 13 , the correction sensitivity S ′ is read from the RAM 42 and the corrected volume difference ΔV of the measured container 17 with respect to the reference container 18 is calculated by the equation (9). Next, the volume difference ΔV is displayed on the display 37 in step S 14 , and the solenoid valve S is displayed in step S 15.
Close V 3 and SV 4, and open solenoid valves SV 5 and SV 6 . T 3 in step S 16
If you start the timer, has elapsed time T 3 step S 17
Then, the indicator 39 is turned over and the measurement is completed. If necessary steps S 13 and wherein the volume V w of the container to be measured 17 between the S 14 (1
The step S ′ 13 calculated by 0) may be provided as shown by the dotted line.

前述したように、被測定容器17の種類、即ちその容積
が変わった場合、基準容器を交換せず容積調整器24を調
整することによって、新しい種類の被測定器17とほぼ等
しい容積の基準容器18を取付けたことと同じになる。従
って必ずしも被測定容器の種類の数だけ基準容器を用意
する必要はなく、容積調整器24を設けることによって用
意しなければならない基準容器の数を減らすことが可能
である。この場合、第4図の感度測定の前に移動調整し
た容器調整器24の容積変化ΔV(c)は第5図の容積測定時
にもそのまま保持しておく必要がある。従って第5図の
ステップS13における測定した容積差は、使用した基準
容器18の容積をV′とすれば、等価基準容積Vm
(V′+ΔV(c))に対する容積差を表わしており、式
(10)は次のように変形される。
As described above, when the type of the container 17 to be measured, that is, its volume is changed, by adjusting the volume adjuster 24 without replacing the reference container, a reference container having a volume substantially equal to that of the new type of device 17 to be measured. It is the same as installing 18. Therefore, it is not always necessary to prepare as many reference containers as the number of types of containers to be measured, and by providing the volume adjuster 24, it is possible to reduce the number of reference containers that must be prepared. In this case, the volume change ΔV (c) of the container adjuster 24, which has been moved and adjusted before the sensitivity measurement shown in FIG. 4, needs to be held as it is during the volume measurement shown in FIG. Therefore the volume difference determined in step S 13 of FIG. 5, if the volume of the reference chamber 18 using the V 'm, the equivalent reference volume V m =
It represents the volume difference with respect to (V ' m + ΔV (c) ), and the equation (10) is transformed as follows.

Vw−(V′+ΔV(c))=ΔV ……(15) 従って被測定容器17の容積を求める場合に第5図のス
テップS′13においてVmの替りに(V′+ΔV(c))を
使って計算する必要がある。勿論、容積調整器24を測定
側空気系に取付けた場合は式(10)においてVwの替りに
(Vw+ΔV(c))を使えばよい。
V w − (V ′ m + ΔV (c) ) = ΔV (15) Therefore, when obtaining the volume of the container 17 to be measured, in step S ′ 13 of FIG. 5, instead of V m , (V ′ m + ΔV ( c) ) must be used for calculation. Of course, when the volume adjuster 24 is attached to the measurement side air system, (V w + ΔV (c) ) may be used instead of V w in the equation (10).

多数の容器について測定を行うにはまず第4図のフロ
ーチャートに示す検出感度Sを求め、あとはそれぞれの
被測定容器について第5図に示す測定を実行すればよ
い。勿論被測定容器ごとに初期タンク圧をPTに正しく設
定すれば第5図におけるステップS4,S5は省略し、ステ
ップS13において補正しない感度Sを使えばよい。
In order to perform the measurement for a large number of containers, first, the detection sensitivity S shown in the flowchart of FIG. 4 is obtained, and thereafter, the measurement shown in FIG. 5 may be executed for each container to be measured. Of course, if the initial tank pressure is properly set to P T for each container to be measured, steps S 4 and S 5 in FIG. 5 may be omitted, and the sensitivity S not corrected in step S 13 may be used.

式(1)で定義しているのは常に測定側空気系と基準
側空気系の容積差であり、従って容積付加器23は測定側
ではなく基準側空気系に取付けてもよい。同様に容積調
整器24も基準側ではなく測定側空気系に取付けてもよ
い。更に容積付加器23と容積調整器24と同じ側に付けて
もよい。容積調整器24は中立点から容積を増加する方に
も減少する方にも調整できるものが好ましい。
What is defined by the equation (1) is always the volume difference between the measurement side air system and the reference side air system. Therefore, the volume adder 23 may be attached to the reference side air system instead of the measurement side. Similarly, the volume adjuster 24 may be attached to the measurement side air system instead of the reference side. Further, the volume adder 23 and the volume adjuster 24 may be provided on the same side. It is preferable that the volume adjuster 24 can be adjusted to increase or decrease the volume from the neutral point.

式(6)における比例定数K=VT(VT+VMは、与
えられたVMに対してVT=VMに選ぶとKが最大となる。即
ちもし測定すべき各容器の堆積がほぼ同じ大きさであれ
ば、あらかじめタンク13,14の容積をVTVMとなるよう
に選んで装置を設計することにより最適感度を得ること
ができる。
The proportionality constant K = V T (V T + V M ) 2 in the equation (6) has a maximum K when V T = V M is selected for a given V M. That is, if the if of each container to be measured is deposited about the same size, it is possible to obtain an optimum sensitivity by designing the device to select the volume of the pre-tanks 13 and 14 so that the V T V M.

「発明の作用効果」 以上説明したように、この発明は気体を使うものであ
って、差圧検出器により被測定容器内の圧力と基準容器
内の圧力との差圧を測定することによって、基準容器に
対する被測定容器の容積差を測定できるようにしたもの
であり、水を使う場合のように大がかりな設備を必要と
せず、また常に基準容積に対して相対的な容積測定を行
うことによって、精度の高い測定を可能にしたものであ
る。
As described above, the present invention uses gas, and by measuring the differential pressure between the pressure in the measured container and the pressure in the reference container by the differential pressure detector, It is designed to measure the volume difference of the measured container with respect to the reference container, does not require large-scale equipment such as when using water, and by always measuring the volume relative to the reference volume. , Which enables highly accurate measurement.

従って、同一仕様の多数の容器の容積のバラツキ測定
などのような極めて高精度を要する測定を行うことがで
き、例えば生産ラインにおける容積測定に好適なもので
ある。
Therefore, it is possible to perform a measurement requiring extremely high accuracy, such as a variation measurement of the volumes of a large number of containers having the same specifications, and it is suitable for volume measurement in a production line, for example.

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

第1図は容積測定装置の機構部を示す図、第2図は容積
測定装置の制御部を示す図、第3図は差圧検出器の時間
に対する出力変化を示す図、第4図は感度測定動作を示
すフローチャート、第5図は容積測定動作を示すフロー
チャートである。 11:圧縮空気源、12:減圧弁、13,14:タンク、15:測定側
配管、16:基準側配管、17:被測定容器、18:基準容器、1
9:差圧検出器、21:圧力計、22:圧力検出器、23:容積付
加器、24:容積調整器、35:メータ型電圧計、SV1〜SV6:
二方電磁弁、SV7:三方電磁弁。
FIG. 1 is a diagram showing a mechanical portion of the volume measuring device, FIG. 2 is a diagram showing a control portion of the volume measuring device, FIG. 3 is a diagram showing an output change of the differential pressure detector with respect to time, and FIG. 4 is a sensitivity. FIG. 5 is a flowchart showing the measuring operation, and FIG. 5 is a flowchart showing the volume measuring operation. 11: Compressed air source, 12: Pressure reducing valve, 13, 14: Tank, 15: Measurement side piping, 16: Reference side piping, 17: Measured container, 18: Reference container, 1
9: Differential pressure detector, 21: Pressure gauge, 22: Pressure detector, 23: Volume adder, 24: Volume adjuster, 35: Meter type voltmeter, SV 1 to SV 6 :
Two-way solenoid valve, SV 7 : Three-way solenoid valve.

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】A 被測定容器側と基準容器側のいずれか
一方に取付けられ、被測定容器側の容積と基準容器側の
容積とをほぼ均衡させる容積調整手段と、 B 互いに等しい容積とされ、互いに等しい圧力の気体
が充填されて前記被測定容器と基準容器とにそれぞれそ
の気体を供給する一対のタンクと、 C 前記被測定容器側と基準容器側のいずれか一方に既
知の容積変化を与える手段と、 D 前記被測定容器内の圧力と前記基準容器内の圧力と
の差圧を測定する手段と、 E 前記容積変化を与えた場合と与えない場合の前記差
圧の変化量と、その与えた容積変化量とから検出感度を
表す容積変化に対する差圧変化の比を算出する手段と、 F 前記差圧と検出感度とから前記基準容器に対する前
記被測定容器の容積差を算出する手段と、 を具備する容積測定装置。
1. A volume adjusting means, which is attached to either one of the measured container side and the reference container side and which substantially balances the measured container side volume and the reference container side volume, and B has the same volume. , A pair of tanks that are filled with gases of equal pressure and supply the gases to the container to be measured and the reference container respectively, and C to a known volume change on either the container to be measured side or the reference container side. Means for giving, D means for measuring the differential pressure between the pressure in the measured container and the pressure in the reference container, E, the amount of change in the differential pressure with and without the volume change, A means for calculating a ratio of a change in differential pressure to a change in volume, which represents detection sensitivity, from the given volume change amount; and a means for calculating a volume difference of the measured container with respect to the reference container from the differential pressure and the detection sensitivity. And is equipped with Product measurement device.
【請求項2】前記タンクの初期圧力を測定する手段と、
前記検出感度を求める時に与えた前記タンクの初期圧力
と、前記容積差を求める時に与えた前記タンクの初期圧
力とから前記検出感度を補正する手段とを含む特許請求
の範囲第1項記載の容積測定装置。
2. Means for measuring the initial pressure of said tank,
2. The volume according to claim 1, further comprising means for correcting the detection sensitivity from the initial pressure of the tank given when the detection sensitivity is obtained and the initial pressure of the tank given when the volume difference is obtained. measuring device.
【請求項3】前記差圧を測定する手段により所定時間を
おいて測定した2つの差圧から前記容積差の算出に用い
る差圧を較正する手段を含む特許請求の範囲第1項記載
の容積測定装置。
3. The volume according to claim 1, further comprising means for calibrating a differential pressure used for calculating the volume difference from two differential pressures measured at a predetermined time by the differential pressure measuring means. measuring device.
【請求項4】等しい圧力の気体が充填された等しい容積
を有する一対のタンクに感度測定用容器及び基準容器を
それぞれ接続導通させ、その導通後におけるそれら感度
測定用容器内圧力と基準容器内圧力との差圧を測定する
ことを、それら感度測定用容器と基準容器のいずれか一
方に既知の容積変化を与えた場合と与えない場合とにつ
いて行う工程と、 その与えた容積変化量と、測定した2つの差圧とから検
出感度を表す容積変化に対する差圧変化の比を算出する
工程と、 等しい圧力の気体が充填された前記一対のタンクに被測
定容器及び前記基準容器をそれぞれ接続導通させる工程
と、 その導通後における前記被測定容器内圧力と基準容器内
圧力との差圧を測定する工程と、 その測定した差圧と前記検出感度とから前記基準容器に
対する前記被測定容器の容積差を算出する工程と、 を含む容積測定方法。
4. A sensitivity measuring container and a reference container are connected and connected to a pair of tanks having an equal volume filled with gas of an equal pressure, and the sensitivity measuring container internal pressure and the reference container internal pressure after the connection are established. Measuring the pressure difference between the sensitivity measurement container and the reference container with or without a known volume change, and with the given volume change amount, the measurement Calculating the ratio of the change in differential pressure to the change in volume, which represents the detection sensitivity, from the two differential pressures, and connecting the measured container and the reference container to the pair of tanks filled with gas of equal pressure, respectively, and connecting them. A step, a step of measuring a differential pressure between the internal pressure of the measured container and a reference internal pressure after the conduction, and the measured differential pressure and the detection sensitivity with respect to the reference container And a step of calculating the volume difference of the container to be measured.
JP62043914A 1987-02-25 1987-02-25 Volume measuring device and its measuring method Expired - Lifetime JPH0812099B2 (en)

Priority Applications (3)

Application Number Priority Date Filing Date Title
JP62043914A JPH0812099B2 (en) 1987-02-25 1987-02-25 Volume measuring device and its measuring method
US07/148,526 US4888718A (en) 1987-02-25 1988-01-26 Volume measuring apparatus and method
KR1019880001587A KR910004621B1 (en) 1987-02-25 1988-02-15 Volume measure system and method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62043914A JPH0812099B2 (en) 1987-02-25 1987-02-25 Volume measuring device and its measuring method

Publications (2)

Publication Number Publication Date
JPS63208720A JPS63208720A (en) 1988-08-30
JPH0812099B2 true JPH0812099B2 (en) 1996-02-07

Family

ID=12676982

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62043914A Expired - Lifetime JPH0812099B2 (en) 1987-02-25 1987-02-25 Volume measuring device and its measuring method

Country Status (1)

Country Link
JP (1) JPH0812099B2 (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP3712761B2 (en) * 1994-06-21 2005-11-02 オルソ−クリニカル ダイアグノスティクス,インコーポレイティド Method for measuring volume of liquid reagent
JP5040128B2 (en) * 2005-04-08 2012-10-03 日産自動車株式会社 Air mixing amount measuring apparatus and air mixing amount measuring method
US11169014B2 (en) * 2019-11-25 2021-11-09 Anton Paar Quantatec, Inc. Bidirectional pycnometer

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4889757A (en) * 1972-02-24 1973-11-22
JPS5484763A (en) * 1977-12-19 1979-07-05 Mitsubishi Electric Corp Volume measuring method and apparatus
JPS5485062A (en) * 1977-12-19 1979-07-06 Mitsubishi Electric Corp Method and apparatus of measuring volume

Also Published As

Publication number Publication date
JPS63208720A (en) 1988-08-30

Similar Documents

Publication Publication Date Title
US4888718A (en) Volume measuring apparatus and method
US4686638A (en) Leakage inspection method with object type compensation
US4670847A (en) Pressure variation detecting type leakage inspection equipment
KR20090003195A (en) Leak test method and leak test device for pipeline
US4523452A (en) Method of measuring leak rates
EP0284262A2 (en) Temperature compensation in differential pressure leak detection
JPS59206737A (en) Leakage testing device having temperature compensating function
JPS6345526A (en) Leak inspection device
US4542643A (en) Fluid leak testing method
US4763518A (en) Method for measuring net internal volume of a receptacle containing an unknown volume of residual liquid
US5207089A (en) Method for measuring the control cross section area of a nozzle
US3893332A (en) Leakage test system
JP4329921B2 (en) Inspection gas mixing apparatus and mixing method
JP2012255687A (en) Pressure leakage measuring method
JPH0812099B2 (en) Volume measuring device and its measuring method
CN102072802B (en) Intelligent constant-voltage high-precision leak detector
JP2000039347A (en) Flowrate inspection device
JP3184885B2 (en) Gas meter calibration device
JP2597710B2 (en) Pressure gauge calibration device
JP3690923B2 (en) Fresh concrete air meter and air amount measuring method
JP3715543B2 (en) Airtight performance test method
JPH0843167A (en) Capacity measuring method of liquid reagent
Boineau et al. Volume calibration using a comparison method with a transfer leak flow rate
JP2618952B2 (en) Calibration device for differential pressure transmitter
JP3186644B2 (en) Gas leak inspection method