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JP3375899B2 - Bypass pipe level gauge - Google Patents
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JP3375899B2 - Bypass pipe level gauge - Google Patents

Bypass pipe level gauge

Info

Publication number
JP3375899B2
JP3375899B2 JP33616498A JP33616498A JP3375899B2 JP 3375899 B2 JP3375899 B2 JP 3375899B2 JP 33616498 A JP33616498 A JP 33616498A JP 33616498 A JP33616498 A JP 33616498A JP 3375899 B2 JP3375899 B2 JP 3375899B2
Authority
JP
Japan
Prior art keywords
pipe
measuring
liquid
reference chamber
tank
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Fee Related
Application number
JP33616498A
Other languages
Japanese (ja)
Other versions
JP2000162020A (en
Inventor
時夫 杉
重忠 松下
満 玉井
繁実 加藤
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.)
Tokyo Keiso Co Ltd
Original Assignee
Tokyo Keiso 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 Tokyo Keiso Co Ltd filed Critical Tokyo Keiso Co Ltd
Priority to JP33616498A priority Critical patent/JP3375899B2/en
Publication of JP2000162020A publication Critical patent/JP2000162020A/en
Application granted granted Critical
Publication of JP3375899B2 publication Critical patent/JP3375899B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Measurement Of Levels Of Liquids Or Fluent Solid Materials (AREA)

Description

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

【0001】[0001]

【発明の属する技術分野】本発明はタンクの側部に取付
けて液面を測定するバイパスパイプ式液面計に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a bypass pipe type liquid level gauge which is attached to a side portion of a tank and measures the liquid level.

【0002】[0002]

【従来の技術とその問題点】貯液タンク内の液体の液面
高さを測定するいわゆるタンク液面計には種々のタイプ
があるが、その中の一種に、図4のような連通管の原理
を用いたバイパスパイプ式(外筒式ともいう)の液面計
がある。
2. Description of the Related Art There are various types of so-called tank level gauges for measuring the level of liquid in a liquid storage tank, one of which is a communication pipe as shown in FIG. There is a bypass pipe type (also called outer cylinder type) level gauge that uses the principle of.

【0003】この方式はタンクの底部、タンクの上部に
設けられた継手管によりタンクと連通する略垂直な測定
管をタンク側面に取付け、このパイプ内の液位を測定す
ることによってタンク内の液位を知るもので、図5のよ
うに上下の継手管部にバルブを取り付けることによって
バルブを閉じれば測定管全体の取り外しが可能なこと、
また、継手管の内径を小さく絞ることによってタンク内
の液面が動揺しても測定管内の液面の動揺が抑制され、
液位の測定が困難にならないことなど、種々の長所があ
り、広く実用に供せられている。
In this system, a substantially vertical measuring pipe communicating with the tank by a joint pipe provided at the bottom of the tank and at the upper part of the tank is attached to the side of the tank, and the liquid level in the pipe is measured to measure the liquid in the tank. It is possible to remove the entire measuring pipe by closing the valve by attaching the valves to the upper and lower joint pipes as shown in Fig. 5,
Also, by squeezing the inner diameter of the joint pipe small, even if the liquid level in the tank fluctuates, the fluctuation of the liquid level in the measuring pipe is suppressed.
It has various advantages, such as the difficulty of measuring the liquid level, and is widely used in practice.

【0004】この「バイパスパイプ式」という分類は、
取付構造上の分類であって、同じ「バイパスパイプ式」
であっても測定管内の液位の測定方法にはさまざまな方
式があり、代表的なものは次の三つである。
This "bypass pipe type" classification is
The same "bypass pipe type" for classification of mounting structure
However, there are various methods for measuring the liquid level in the measuring tube, and the following three methods are typical.

【0005】・透明な測定管を用いて外部から液面を直
視するいわゆるサイトグラス式。 ・測定管の液中に、マグネット内蔵のフロートを浮か
べ、フロートの位置(高さ)をパイプの側方から磁気検
出形位置センサにて検知して液位を求めるいわゆるバイ
パスフロート式(図6)。 ・測定管の液中に、液よりも見かけ比重(重さ÷体積)
の大きい液面感得体(ディスプレーサ)を吊り下げ、液
面感得体に働く浮力を検出して液位を求めるいわゆるデ
ィスプレースメント式(図7)。
A so-called sight glass type in which the liquid surface is directly viewed from the outside by using a transparent measuring tube.・ A so-called bypass float system (Fig. 6) in which a float with a built-in magnet is floated in the liquid of the measuring pipe and the position (height) of the float is detected from the side of the pipe by a magnetic detection type position sensor to obtain the liquid level. .・ Apparent specific gravity (weight ÷ volume) in the liquid of the measuring tube
A so-called displacement type (Fig. 7) in which a liquid level sensitizer (displacer) having a large value is suspended and the buoyancy acting on the liquid level sensitizer is detected to determine the liquid level.

【0006】これらの方式のものではそれぞれ長所、短
所があり、目的に応じて選択使用されているが、サイト
グラス式は測定管の強度、耐久性が金属パイプに比べて
劣ることから、測定管が破損して液が流出しても危険性
の小さいタンクに限られる。
[0006] Each of these methods has advantages and disadvantages and is selectively used according to the purpose. However, the sight glass method is inferior in strength and durability to the measuring tube, and therefore the measuring tube is inferior to the metal tube. It is limited to tanks where there is little danger even if the liquid breaks out and liquid leaks out.

【0007】バイパスフロート式、ディスプレースメン
ト式はパイプが金属製で完全密閉構造にすることができ
るため、安全性の面では優れているが、測定管の中に可
動部を有するため、長期の耐久性や、液が異常に動揺し
た際の保全に関しては問題があり、可動部を持たない方
式の「バイパスパイプ式液面計」の実現がユーザから強
く望まれている。
[0007] The bypass float type and displacement type are excellent in safety because the pipe is made of metal and can have a completely closed structure, but it has a movable part in the measuring pipe, so it has long-term durability. There is a problem with respect to the property and maintenance when the liquid is shaken abnormally, and there is a strong demand from the users to realize a "bypass pipe type liquid level gauge" that does not have a moving part.

【0008】可動部のない一般的な液面計には、(1)
超音波式、(2)電波式、(3)光学式の3方式のもの
があるが、バイパスパイプ式液面計へ適用するにはそれ
ぞれ次ぎのような問題点があり、実用化には至ってな
い。
For a general liquid level gauge having no moving parts, (1)
There are three types, ultrasonic type, (2) radio type, and (3) optical type, but each has the following problems when applied to the bypass pipe type level gauge, and it has not been put to practical use. Absent.

【0009】すなわち、(1)の超音波式では、原理的
に超音波の伝播速度(音速)が液位を求める上で既知で
なければならないが、音速は伝播物質の温度、密度に大
きく依存する。
That is, in the ultrasonic method (1), in principle, the propagation velocity (sonic velocity) of ultrasonic waves must be known in order to obtain the liquid level, but the velocity of sound greatly depends on the temperature and density of the propagating substance. To do.

【0010】バイパスパイプ式液面計の適用対象の多く
は密閉タンクであり、タンク内の圧力、温度が一定でな
いため、タンク頂から液面までの空間を超音波が往復す
るのに要する時間によって液位を求める通常の超音波液
面計の測定方式では、別途に温度、圧力を測定して空間
の音速を正確に推定しない限り精度が悪く、実用にはな
らない。したがって温度計、圧力計、音速の推定計算回
路などを付加せねばならず、コストが大幅に上昇する。
Most of the objects to which the bypass pipe type liquid level gauge is applied are closed tanks, and since the pressure and temperature in the tank are not constant, depending on the time required for ultrasonic waves to reciprocate in the space from the tank top to the liquid level. In the conventional ultrasonic liquid level gauge measuring method for obtaining the liquid level, the accuracy is poor and practically useless unless the temperature and pressure are separately measured to accurately estimate the sound velocity in the space. Therefore, a thermometer, a pressure gauge, a sound velocity estimation calculation circuit, and the like must be added, which significantly increases the cost.

【0011】一方、(2)の電波式は超音波式と異な
り、伝播速度は温度、密度によって影響を受けることは
殆どなく、オープンな空間では高精度の液面計として実
用化されている。
On the other hand, the radio wave method (2) is different from the ultrasonic wave method in that the propagation velocity is hardly affected by the temperature and the density, and is practically used as a highly accurate liquid level gauge in an open space.

【0012】しかし、測定管が金属製の場合、内径が小
さく、かつ内面の曲率の大きい測定管では、液面からの
直接の反射波と測定管内面を経由する間接反射波の弁別
が技術的に難しいこと、測定管が非金属の場合、電波が
外部に放射されて、他の電子機器に障害を与える恐れが
あること、超音波式に比べてコストが高いこと、などの
理由により実用化されたものはない。
However, when the measuring pipe is made of metal, it is technically possible to discriminate between the direct reflected wave from the liquid surface and the indirect reflected wave passing through the inner surface of the measuring pipe in the measuring pipe having a small inner diameter and a large inner curvature. It is difficult to use, and if the measuring tube is non-metallic, radio waves may be radiated to the outside, which may interfere with other electronic devices, and the cost is higher than the ultrasonic type. There was nothing that was done.

【0013】また、(3)の光学式はレンズ系で光束を
任意に調節できるため、電波式のような反射波弁別の難
しさはないが、発光部、受光部の液の結露やゴミの付着
に弱いこと、しかも液面のわずかな動揺で反射光が減衰
することなど、測定環境に関する制約が多く、適用対象
が限られる。
In the optical system of (3), since the light flux can be arbitrarily adjusted by the lens system, there is no difficulty in discriminating the reflected waves as in the radio wave system, but condensation of liquid and dust of the light emitting portion and the light receiving portion can be prevented. There are many restrictions on the measurement environment, such as weak adhesion, and a slight fluctuation of the liquid surface that attenuates the reflected light.

【0014】[0014]

【目的】本発明は、タンクの上部と底部の継手管を介し
てタンクの側面に取り付けられ、タンク内と連通する略
垂直な測定管(いわゆるバイパス形測定管)内の液位
を、同パイプ内に可動部を用いない方法で測定してタン
ク内の液位を求めるコストの安いバイパスパイプ式液面
計を提供できるようにした。
[Purpose] The present invention is to attach a liquid level in a substantially vertical measuring pipe (so-called bypass type measuring pipe), which is attached to the side surface of the tank through joint pipes at the top and bottom of the tank and communicates with the inside of the tank. A low-cost bypass pipe type liquid level gauge for measuring the liquid level in a tank by measuring without using a movable part is provided.

【0015】[0015]

【本発明の手段】本発明の液面計は、タンク内へ継手管
にてバイパス連通せしめてタンクの側方に設ける測定管
の下部側方に、同測定管内と連通し、かつこの測定管よ
りも高さ低い基準室側管を設けて、測定管及び基準室
側管の各底部に、各底部から液中に発信されて測定管内
の液面で反射された超音波信号を受信する信号送・受信
素子と、基準室側管内の上部内面で反射された超音波信
号を受信する信号送・受信素子をそれぞれ設けたものと
してある。数である高さaとから、タンク内の液位Lを L=a・t2/t1 の演算で求める制御演算回路に接続したものとしてあ
る。
The liquid level gauge of the present invention is constructed such that a bypass pipe is connected to the inside of a tank by bypass connection and the lower part of the measuring pipe provided on the side of the tank is connected to the inside of the measuring pipe. provided low reference chamber side pipe height than, the respective bottom of the measuring tube and the reference chamber side tube, receives the ultrasonic signal reflected by the liquid surface of the measuring tube is originated in the liquid from the bottom A signal transmission / reception element and a signal transmission / reception element for receiving the ultrasonic signal reflected on the inner surface of the upper portion of the reference chamber side tube are provided. It is assumed that the liquid level L in the tank is connected to a control arithmetic circuit which is calculated by the equation L = a · t 2 / t 1 from the height a which is a number.

【0016】より具体的には、測定管及び基準室側管の
各底部に、一対の超音波送信素子と受信素子設けるか、
あるいは1個で送信と受信の機能を備える圧電素子をそ
れぞれ設けたものとしてある。
More specifically, a pair of ultrasonic transmitting element and receiving element are provided at the bottom of each of the measuring tube and the reference chamber side tube, or
Alternatively, one piezoelectric element having a transmission function and a piezoelectric element having a reception function is provided.

【0017】また、信号送・受信素子は制御演算回路に
接続し、この回路では、測定管の底部から発信された超
音波信号が測定管内の液面で反射されて底部の送・受信
素子に達するまでの時間t2と、基準室側管の底部から
発信された超音波信号が基準室側管内の上部内面で反射
して底部の信号送・受信素子に達するまでの時間t1
検出し、基準室側管における底部の信号送・受信素子面
から上部内面までの定数である高さaとから、タンク内
の液位Lを L=a・t2/t1 の演算で求める制御演算回路に接続したものとしてあ
る。
Further, the signal transmitting / receiving element is connected to a control arithmetic circuit. In this circuit, the ultrasonic signal transmitted from the bottom of the measuring tube is reflected by the liquid surface in the measuring tube and is transmitted to the transmitting / receiving element at the bottom. and the time t 2 to reach, to detect the time t 1 until the ultrasonic signal transmitted from the bottom of the reference chamber side pipe reaches the signal transmitting receiving device at the bottom and reflected by the upper inner surface of the reference chamber side pipe , A control calculation for obtaining the liquid level L in the tank by the calculation of L = a · t 2 / t 1 from the height a which is a constant from the signal transmitting / receiving element surface at the bottom of the reference chamber side tube to the upper inner surface. It is supposed to be connected to a circuit.

【0018】[0018]

【実施例】<実施例1>図1のように、上側部と下側部
にタンク内へ連通せしめる継手管1a,1bを有するバ
イパス用の測定管1の下端に、上方に向かって超音波を
放射する素子3aと、上方から入射する超音波を検出す
る素子3bをそれぞれ設ける。
<Example 1> As shown in FIG. 1, ultrasonic waves are directed upwards at the lower end of a bypass measuring pipe 1 having joint pipes 1a and 1b for communicating with the inside of a tank on the upper side and the lower side. The element 3a for radiating the light and the element 3b for detecting the ultrasonic wave incident from above are respectively provided.

【0019】測定管1の下部側方には、基準室となるバ
イパス基準室側管2を、その上側部と下側部を連通部2
a,2bで測定管1内と導通せしめて設け、この基準室
側管2の内底面は測定管1の内底面と同一面としてあ
る。この基準室側管2の下部にも超音波を放射する素子
4a、入射する超音波を検出する素子4bを設けてあ
る。なお、基準室側管2は測定管1の外側方の任意の位
置に設ければよい。
A bypass reference chamber side pipe 2 serving as a reference chamber is provided on the lower side of the measuring pipe 1, and an upper portion and a lower portion of the bypass reference chamber side pipe 2 communicate with each other.
The reference chamber side tube 2 has an inner bottom surface flush with the inner bottom surface of the measuring tube 1. An element 4a for emitting an ultrasonic wave and an element 4b for detecting an incident ultrasonic wave are also provided below the reference chamber side tube 2. The reference chamber side tube 2 may be provided at an arbitrary position outside the measurement tube 1.

【0020】継手管でタンクの側方部に取り付けたバイ
パス用の測定管1内の液面が上方にある場合、同パイプ
下端の超音波を放射する素子3aから上方に超音波を放
射(発信)させると、超音波は測定管内の液中を伝播す
る。超音波は液面まで進み、液面で反射されて測定管内
を下方に伝播し、測定管下端に戻り、これを検出素子3
bが検出する。
When the liquid level in the bypass measuring pipe 1 attached to the side of the tank with the joint pipe is upward, the ultrasonic wave is emitted upward from the ultrasonic wave emitting element 3a at the lower end of the pipe. ), The ultrasonic wave propagates in the liquid in the measuring tube. The ultrasonic wave propagates to the liquid surface, is reflected by the liquid surface, propagates downward in the measuring pipe, returns to the lower end of the measuring pipe, and detects the detection element 3
b detects.

【0021】一方、基準室側管2の下端部に設けた超音
波を放射する素子4aから上部の反射面2c(基準室側
管の上部内面)に向けて超音波を放射(発信)させる
と、超音波は基準室側管内の液中を伝播し、前記反射面
2cで反射されて基準室側管の端部に戻り、これを検出
素子4bが検出する。
On the other hand, when the ultrasonic wave is emitted (transmitted) from the ultrasonic wave radiating element 4a provided at the lower end of the reference chamber side tube 2 toward the upper reflecting surface 2c (the upper inner surface of the reference chamber side tube). , The ultrasonic wave propagates through the liquid in the reference chamber side tube, is reflected by the reflecting surface 2c and returns to the end portion of the reference chamber side tube, and this is detected by the detection element 4b.

【0022】図3は超音波放射素子3a、4aに印加し
たパルス状電圧と、検出素子3b、4bが反射波を受信
したときの出力電圧の一例である。同図に示すように、
基準室側管2の底部放射素子4aから発信した超音波が
同側管2の上部反射面2cで反射されて検出素子4bが
受信するまでの時間をt1、測定管1の底部放射素子3
aから発信した超音波が同測定管内の液面で反射されて
検出素子3bが受信するまでの時間をt2 とすると、基
準室側管2の素子(4a,4b)から反射面2c(同パ
イプの上部内面)までの距離は一定で既知であるから、
その距離をaとすると、 V×t1 =2a V×t2 =2L (V:超音波の伝播速度、L:素子から液面までの距
離)となる。
FIG. 3 shows an example of the pulsed voltage applied to the ultrasonic wave radiating elements 3a and 4a and the output voltage when the detecting elements 3b and 4b receive the reflected wave. As shown in the figure,
The time until the ultrasonic wave emitted from the bottom radiating element 4a of the reference chamber side tube 2 is reflected by the upper reflecting surface 2c of the same side tube 2 and is received by the detecting element 4b is t 1 , and the bottom radiating element 3 of the measuring tube 1 is
When the time until the ultrasonic wave transmitted from a is reflected by the liquid surface in the same measuring tube and received by the detecting element 3b is t 2 , the element (4a, 4b) of the reference chamber side tube 2 reflects from the reflecting surface 2c (the same). Since the distance to the upper inner surface of the pipe) is constant and known,
If the distance is a, then V × t 1 = 2a V × t 2 = 2L (V: ultrasonic propagation velocity, L: distance from element to liquid surface).

【0023】したがって、測定管1内の底部素子(3
a,3b)の位置を基準にした液位Lは L=a×t2 /t1 ・・・・・・・(I) の演算により求められる。
Therefore, the bottom element (3
The liquid level L based on the positions a, 3b) is obtained by the calculation of L = a × t 2 / t 1 ... (I).

【0024】しかして超音波の伝播速度が変化してもそ
の影響を受けないし、素子と測定管内の液の間の隔壁を
超音波が伝播する速度は、一般に液の音速Vと同じでは
ないが、隔壁が著しく厚くないならば、上記の計算式で
生じる音速の違いによる誤差はわずかで無視できる。
However, even if the propagation speed of the ultrasonic wave is changed, it is not affected, and the speed at which the ultrasonic wave propagates through the partition wall between the element and the liquid in the measuring tube is not generally the same as the sound velocity V of the liquid. If the partition wall is not extremely thick, the error due to the difference in sound velocity generated by the above calculation formula is negligible and can be ignored.

【0025】上記演算は例えば図示のごとき切換回路、
発信回路、受信回路、測定・演算回路を備える制御演算
回路で次のように行われる。 (1) 測定回路からの制御信号によって駆動される切換回
路7bによって放射素子4aに発信回路を接続するとと
もに切換回路7aによって検出素子4bに受信回路を接
続し、前記発信回路により放射素子4aにパルス状の電
圧を印加して超音波を発信させる。放射素子4aから液
中に発信された超音波は、基準室側管2の反射面に到達
し、ここで反射されて下方に伝播する。 (2) 測定回路は、発信回路が放射素子4aにパルス状電
圧を印加した瞬間にタイマーをスタートさせる。 (3) 上記の下方に伝播する超音波を検出素子4bにより
受信する。この時受信回路によって検出される電気信号
は検出素子の出力を増幅したものであり、その波形は図
3と同様になる。 (4) 測定回路は、受信回路が基準室側管の反射面からの
超音波を受信した瞬間にタイマーをストップさせ、伝播
時間t1 を計測する。 (5) 切換回路7bによって放射素子3aを発信回路に接
続するとともに切換回路7aによって検出素子3bを受
信回路に接続し、前記(1) 〜(4) と同様の手順を放射素
子3aおよび検出素子3bについて行って、測定管の液
面から反射された超音波の伝播時間t2 を計測する。 (6) 測定回路は、(4) および(5)で得たt1 および
2 を前記の計算式(I)に代入して放射素子および検
出素子から測定管内の液面までの距離Lを求める。測定
管内の液位はタンクの液位に常に等しいから、タンクの
液位を次式(II)によって得る。 タンクの液位=L−h ・・・・・(II) h;素子の表面と液位0平面との距離
The above calculation is performed by a switching circuit as shown in the figure,
A control arithmetic circuit including a transmitting circuit, a receiving circuit, and a measuring / arithmetic circuit is used as follows. (1) A switching circuit 7b driven by a control signal from a measurement circuit connects a radiating element 4a with a transmitting circuit, and a switching circuit 7a connects a detecting circuit with a receiving circuit, and the transmitting circuit outputs a pulse to the radiating element 4a. The ultrasonic wave is emitted by applying a voltage of the form. The ultrasonic wave transmitted from the radiating element 4a into the liquid reaches the reflecting surface of the reference chamber side tube 2, is reflected here, and propagates downward. (2) The measuring circuit starts the timer at the moment when the transmitting circuit applies the pulsed voltage to the radiating element 4a. (3) The ultrasonic wave propagating downward is received by the detecting element 4b. At this time, the electric signal detected by the receiving circuit is an amplified output of the detection element, and its waveform is similar to that shown in FIG. (4) The measuring circuit stops the timer at the moment when the receiving circuit receives the ultrasonic wave from the reflecting surface of the reference chamber side tube, and measures the propagation time t 1 . (5) The radiating element 3a is connected to the transmitting circuit by the switching circuit 7b, the detecting element 3b is connected to the receiving circuit by the switching circuit 7a, and the same procedure as in (1) to (4) above is performed. 3b, the propagation time t 2 of the ultrasonic wave reflected from the liquid surface of the measuring tube is measured. (6) The measuring circuit substitutes t 1 and t 2 obtained in (4) and (5) into the above calculation formula (I) to calculate the distance L from the radiating element and the detecting element to the liquid level in the measuring tube. Ask. Since the liquid level in the measuring pipe is always equal to the liquid level in the tank, the liquid level in the tank is obtained by the following equation (II). Liquid level of tank = L−h (II) h; Distance between element surface and liquid level 0 plane

【0026】<実施例2>圧電素子の場合、パルス電圧
を印加することにより超音波を放射する機能と、入射さ
れた超音波を検知する機能とを兼ね備えているので、切
換回路によって発信回路と受信回路のどちらか一方を素
子に接続するようにすれば、1個の圧電素子で両機能を
実現することができるので、その実施例を図2に示す。
<Embodiment 2> In the case of a piezoelectric element, since it has both the function of emitting ultrasonic waves by applying a pulse voltage and the function of detecting the incident ultrasonic waves, the switching circuit serves as an oscillator circuit. If one of the receiving circuits is connected to the element, both functions can be realized by one piezoelectric element, and an example thereof is shown in FIG.

【0027】同図に示すように、バイパス測定管1の下
端及び基準室側管2の下端にそれぞれ圧電素子5A,5
Bを密着させて固定する。図ではスプリング6で押し付
けているが、接着してもよい。
As shown in the figure, piezoelectric elements 5A and 5A are provided at the lower end of the bypass measuring pipe 1 and the lower end of the reference chamber side pipe 2, respectively.
Fix B closely. Although it is pressed by the spring 6 in the figure, it may be adhered.

【0028】圧電素子5A、5Bには切換回路、発信回
路と受信回路、測定・演算回路からなる制御演算回路に
接続されていて、圧電素子5A、5Bは切換により超音
波の発信、受信の何れかを行い、液位測定は制御演算回
路により次ぎのように行われる。 (1) 測定回路からの制御信号によって駆動される切換回
路7aおよび7bによって圧電素子5Bに発信回路を接
続し、圧電素子5Bにパルス状の電圧を印加して超音波
を発信させる。 (2) 圧電素子5Bに接続する回路を切換回路7bにより
受信回路に切換え、基準室側管2の反射面に到達して反
射された超音波を圧電素子により受信し、伝播時間t1
を計測する。 (3) 前記(1)、(2) と同様に圧電素子5Aを発信回路、
受信回路に順次接続して、伝播時間t2 を計測する。 (4) 測定回路は、(1) 〜(3) で得た伝播時間t1 、t2
から前記計算式(I)により液面までの距離Lを求め、
さらに前記(II)式によってタンクの液位を得る。
The piezoelectric elements 5A and 5B are connected to a control arithmetic circuit composed of a switching circuit, a transmitting circuit and a receiving circuit, and a measurement / arithmetic circuit. The piezoelectric elements 5A and 5B are switched to transmit or receive ultrasonic waves. Then, the liquid level is measured by the control arithmetic circuit as follows. (1) An oscillation circuit is connected to the piezoelectric element 5B by switching circuits 7a and 7b driven by a control signal from the measurement circuit, and a pulse voltage is applied to the piezoelectric element 5B to emit ultrasonic waves. (2) The circuit connected to the piezoelectric element 5B is switched to the receiving circuit by the switching circuit 7b, and the ultrasonic wave that reaches the reflecting surface of the reference chamber side tube 2 and is reflected by the piezoelectric element is received, and the propagation time t 1
To measure. (3) As in (1) and (2) above, the piezoelectric element 5A is used as an oscillator circuit,
The propagation time t 2 is measured by sequentially connecting to the receiving circuit. (4) The measurement circuit uses the propagation times t 1 and t 2 obtained in (1) to (3).
From the above, the distance L to the liquid surface is obtained by the above calculation formula (I),
Further, the liquid level in the tank is obtained by the above formula (II).

【0029】[0029]

【発明の効果】本発明は可動部がないため、長期の耐久
性や、液が異常に動揺した際の保全に関しては殆ど問題
がなく、ユーザから強く要望されている可動部を持たな
い方式の「バイパスパイプ式液面計」を提供できる。
EFFECTS OF THE INVENTION Since the present invention has no moving parts, there is almost no problem in terms of long-term durability and maintenance in the case where liquid is shaken abnormally. A "bypass pipe type liquid level gauge" can be provided.

【0030】バイパスパイプ式液面計の適用対象の多く
は密閉タンクであり、タンク内の圧力、温度が一定でな
いため、タンク頂から液面までの空間を超音波が往復す
るのに要する時間によって液位を求める従来の超音波液
面測定方式では、別途に温度、圧力を測定して空間の音
速を正確に推定しない限り精度が悪く、したがって温度
計、圧力計、音速の推定計算回路などを付加せねばなら
ず、コストが大幅に上昇するが、本発明は、検出信号が
液中の伝播信号だけであり、タンク頂から液面までの空
間を超音波が往復するのに要する時間によって液位を求
めるものではないので、温度計、圧力計、音速の推定計
算回路などを付加する必要はなく、製造コストの大幅低
減が期せる。
Most of the objects to which the bypass pipe type liquid level gauge is applied are closed tanks, and since the pressure and temperature in the tank are not constant, it depends on the time required for the ultrasonic waves to reciprocate in the space from the tank top to the liquid level. The conventional ultrasonic liquid level measurement method for determining the liquid level is inaccurate unless the temperature and pressure are separately measured and the sound velocity in the space is accurately estimated. Therefore, a thermometer, a pressure gauge, a sound velocity estimation calculation circuit, etc. However, in the present invention, the detection signal is only a propagation signal in the liquid, and the ultrasonic wave reciprocates in the space from the tank top to the liquid surface depending on the time required for the liquid to flow. Since it is not required to calculate the unit, it is not necessary to add a thermometer, a pressure gauge, a sound velocity estimation calculation circuit, etc., and the manufacturing cost can be greatly reduced.

【0031】また、伝播時間t1 からタンク内液の超音
波伝播速度Vを知ることができるので、タンク内液の温
度、濃度(薬液の場合)など、伝播速度Vに依存タンク
内液の物理量をも同時に求めることができるという付加
的利点もある。
Further, since the ultrasonic wave propagation speed V of the liquid in the tank can be known from the propagation time t 1 , the physical quantity of the liquid in the tank depends on the temperature, concentration (in the case of chemical liquid) of the liquid in the tank, and the propagation speed V. Also has the additional advantage that it can be obtained at the same time.

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

【図1】本発明に係る液面計をタンクに装着した状態を
示す縦断面図。
FIG. 1 is a vertical cross-sectional view showing a state in which a liquid level gauge according to the present invention is attached to a tank.

【図2】本発明に係る他の実施例の液面計をタンクに装
着した状態を示す縦断面図。
FIG. 2 is a vertical cross-sectional view showing a state in which a liquid level gauge according to another embodiment of the present invention is attached to a tank.

【図3】素子への印加電圧と受信による素子の出力電圧
の一例を示すグラフ。
FIG. 3 is a graph showing an example of an applied voltage to an element and an output voltage of the element due to reception.

【図4】従来のバイパスパイプ式液面計の一例を示す縦
断面図。
FIG. 4 is a vertical sectional view showing an example of a conventional bypass pipe type liquid level gauge.

【図5】従来のバイパスパイプ式液面計の他の例を示す
縦断面図。
FIG. 5 is a vertical cross-sectional view showing another example of a conventional bypass pipe type liquid level gauge.

【図6】従来のバイパスパイプ式(バイパスフロート
式)液面計の例を示す縦断面図。
FIG. 6 is a vertical cross-sectional view showing an example of a conventional bypass pipe type (bypass float type) liquid level gauge.

【図7】従来のバイパスパイプ式(ディスプレースメン
ト式)液面計の一例を示す縦断面図。
FIG. 7 is a vertical cross-sectional view showing an example of a conventional bypass pipe type (displacement type) level gauge.

【符号の説明】[Explanation of symbols]

1 測定管 2 基準室側管 3a 超音波放射素子 3b 超音波検出素子 4a 超音波放射素子 4b 超音波検出素子 5A、5B 圧電素子 6 スプリング 7a,7b 切換回路 1 Measuring tube 2 Reference chamber side tube 3a Ultrasonic radiating element 3b Ultrasonic detecting element 4a ultrasonic radiating element 4b ultrasonic detecting element 5A, 5B Piezoelectric element 6 Spring 7a, 7b switching circuit

───────────────────────────────────────────────────── フロントページの続き (72)発明者 加藤 繁実 東京都板橋区相生町1−13−309 (56)参考文献 特開 昭51−75557(JP,A) 特開 平8−145763(JP,A) 特公 昭35−4380(JP,B1) (58)調査した分野(Int.Cl.7,DB名) G01F 23/00 - 25/00 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Shigemi Kato 1-13-309 Aioicho, Itabashi-ku, Tokyo (56) References JP-A-51-75557 (JP, A) JP-A-8-145763 (JP, A) Japanese Patent Publication Sho 35-4380 (JP, B1) (58) Fields investigated (Int.Cl. 7 , DB name) G01F 23 / 00-25 / 00

Claims (2)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】タンク内へ継手管にてバイパス連通せしめ
てタンクの側方に設ける測定管の下部側方に、同測定管
内と連通し、かつこの測定管よりも高さ低い基準室側
管を設けて、測定管及び基準室側管の各底部に、各底部
から液中に発信されて測定管内の液面で反射された超音
波信号を受信する信号送・受信素子と、基準室側管内の
上部内面で反射された超音波信号を受信する信号送・受
信素子をそれぞれ設けてなるバイパスパイプ式液面計。
1. A reference chamber side, which communicates with the inside of the measuring pipe and is lower in height than the measuring pipe, which is connected to the inside of the measuring pipe by bypass connection to the inside of the tank and is provided on the side of the tank. A pipe is provided to each of the bottoms of the measurement pipe and the reference chamber side pipe, and a signal transmission / reception element that receives the ultrasonic signal transmitted from the bottom into the liquid and reflected by the liquid surface in the measurement pipe, and the reference chamber. A bypass pipe type level gauge provided with signal transmitting / receiving elements for receiving ultrasonic signals reflected by the upper inner surface of the side pipe.
【請求項2】タンク内へ継手管にてバイパス連通せしめ
てタンクの側方に設ける測定管の下部側方に、同測定管
内と連通し、かつこの測定管よりも高さ低い基準室側
管を設けて、測定管及び基準室側管の各底部に、各底部
から液中に発信されて測定管内の液面で反射された超音
波信号を受信する信号送・受信素子と、基準室側管内の
上部内面で反射された超音波信号を受信する信号送・受
信素子をそれぞれ設け、これらの信号送・受信素子を、
測定管底部の信号送・受信素子から測定管の液中に発し
た超音波信号が測定管内の液面で反射して測定管底部の
信号送・受信素子に達するまでの時間t2と、基準室側
管底部の信号送・受信素子から基準室側管の液中に発し
た超音波信号が基準室側管内の上部内面で反射して基準
室側管底部の信号送・受信素子に達するまでの時間t1
と、基準室側管における信号送・受信素子面から上部内
面までの定数である高さaとから、タンク内の液位Lを L=a・t2/t1 の演算で求める制御演算回路に接続してなるバイパスパ
イプ式液面計。
2. A reference chamber side, which communicates with the inside of the measuring pipe and is lower in height than the measuring pipe, is connected to the lower side of the measuring pipe which is provided on the side of the tank by bypass communication with the inside of the tank. A pipe is provided to each of the bottoms of the measurement pipe and the reference chamber side pipe, and a signal transmission / reception element that receives the ultrasonic signal transmitted from the bottom into the liquid and reflected by the liquid surface in the measurement pipe, and the reference chamber. Each of the signal transmitting / receiving elements for receiving the ultrasonic signal reflected by the inner surface of the upper portion of the side tube is provided, and these signal transmitting / receiving elements are
Time t 2 from the signal transmitting / receiving element at the bottom of the measuring tube to the signal transmitting / receiving element at the bottom of the measuring tube after the ultrasonic signal generated in the liquid in the measuring tube is reflected by the liquid surface in the measuring tube Until the ultrasonic signal emitted from the signal sending / receiving element at the bottom of the chamber side tube into the liquid in the reference chamber side tube is reflected by the upper inner surface of the tube inside the reference chamber side and reaches the signal sending / receiving element at the bottom of the reference chamber side tube. Time t 1
And a height a which is a constant from the signal transmitting / receiving element surface in the reference chamber side pipe to the upper inner surface, a control calculation circuit for calculating the liquid level L in the tank by calculation of L = a · t 2 / t 1. Bypass pipe type level gauge connected to.
JP33616498A 1998-11-26 1998-11-26 Bypass pipe level gauge Expired - Fee Related JP3375899B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP33616498A JP3375899B2 (en) 1998-11-26 1998-11-26 Bypass pipe level gauge

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP33616498A JP3375899B2 (en) 1998-11-26 1998-11-26 Bypass pipe level gauge

Publications (2)

Publication Number Publication Date
JP2000162020A JP2000162020A (en) 2000-06-16
JP3375899B2 true JP3375899B2 (en) 2003-02-10

Family

ID=18296343

Family Applications (1)

Application Number Title Priority Date Filing Date
JP33616498A Expired - Fee Related JP3375899B2 (en) 1998-11-26 1998-11-26 Bypass pipe level gauge

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Country Link
JP (1) JP3375899B2 (en)

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE10312102B4 (en) * 2003-03-19 2015-10-08 Robert Bosch Gmbh Device for measuring a level of a liquid in a container
US9020767B2 (en) * 2011-11-21 2015-04-28 The Boeing Company Wireless fuel monitoring system
CN103292867A (en) * 2013-05-13 2013-09-11 江苏杰创科技有限公司 External non-contact measurement barrel type ultrasonic liquid level meter
DE102022208284B3 (en) 2022-08-09 2023-12-28 Vitesco Technologies GmbH Fluid container and fluid container device for fluids

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