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JPH0778445B2 - Ultrasonic interface level meter - Google Patents
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JPH0778445B2 - Ultrasonic interface level meter - Google Patents

Ultrasonic interface level meter

Info

Publication number
JPH0778445B2
JPH0778445B2 JP2319537A JP31953790A JPH0778445B2 JP H0778445 B2 JPH0778445 B2 JP H0778445B2 JP 2319537 A JP2319537 A JP 2319537A JP 31953790 A JP31953790 A JP 31953790A JP H0778445 B2 JPH0778445 B2 JP H0778445B2
Authority
JP
Japan
Prior art keywords
wave
ultrasonic
medium
container
shell wall
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
JP2319537A
Other languages
Japanese (ja)
Other versions
JPH04188028A (en
Inventor
靖史 那須
耕司 戸田
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.)
Canon Finetech Nisca Inc
Original Assignee
Nisca 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 Nisca Corp filed Critical Nisca Corp
Priority to JP2319537A priority Critical patent/JPH0778445B2/en
Publication of JPH04188028A publication Critical patent/JPH04188028A/en
Publication of JPH0778445B2 publication Critical patent/JPH0778445B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime 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】 [産業上の利用分野] 本発明は容器内の気体、液体、粉粒体、ゲル状物質等の
相互の界面レベルを検知する超音波界面レベル計に関
し、特に容器外部から、該容器に機械的の加工を施すこ
となく取り付け容器内の媒体を検出する場合に最も敵す
る。
Description: [Industrial application] The present invention relates to an ultrasonic interface level meter for detecting the mutual interface level of a gas, a liquid, a granular material, a gel-like substance or the like in a container, and particularly to the outside of the container. Therefore, it is most suitable for detecting the medium in the mounting container without mechanically processing the container.

[従来の技術] 従来、この種の超音波界面レベル計の一つとして、容器
内の液面を検知する超音波液面計が知られている。この
超音波液面計の中で、特に容器外部から、該容器に機械
的の加工を施すことなく内容液の液面を検知可能なもの
としては、例えば特開昭60−214226号公報、特開昭61−
29722号公報、特開昭60−262019号公報(以下、この順
序で第1公報、第2公報、第3公報と称する。)などに
開示されたものがある。
[Prior Art] Conventionally, as one of the ultrasonic interface level meters of this type, an ultrasonic liquid level meter that detects a liquid level in a container is known. Among the ultrasonic level gauges, those capable of detecting the liquid level of the content liquid, particularly from the outside of the container, without subjecting the container to mechanical processing are disclosed in, for example, JP-A-60-214226. Kai 61-
There are those disclosed in Japanese Patent No. 29722, Japanese Patent Laid-Open No. 60-262019 (hereinafter referred to as the first, second, and third publications in this order).

しかして、前記第1公報のものは、送波器と受波器とを
容器の一水平横断面内の対向位置に取り付けておき、送
波器から投入された超音波を受波器で検出して液面を測
定するものである。
In the device of the first publication, the wave transmitter and the wave receiver are attached at opposite positions in one horizontal cross section of the container, and the ultrasonic wave input from the wave detector is detected by the wave receiver. Then, the liquid level is measured.

また、第2公報のものでは、送受波機能一体の液面計を
容器外壁に取り付け、壁面を通して液中に放射された超
音波が対向する壁面に反射して帰還した反射波を受信し
て液の有無を知ろうとするものである。
In the second publication, a liquid level gauge integrated with a wave transmission / reception function is attached to the outer wall of the container, and the ultrasonic wave radiated into the liquid through the wall is reflected by the opposite wall to receive the reflected wave and the liquid is received. It is intended to know the presence or absence of.

さらに前記第3公報のものは、やはり送受波機能一体の
液面計を容器外壁に取り付け、外壁面かち入射した超音
波が内壁面に当たって反射する多重反射(多重エコー)
が内壁面に液体が接しているか否かによってエコーの持
続時間が異なるのを利用して内容液の有無を知ろうとす
るものである。
Further, in the third publication, a liquid level gauge having an integrated wave transmitting / receiving function is attached to the outer wall of the container, and the ultrasonic wave incident on the outer wall hits the inner wall and is reflected.
It is intended to know the presence or absence of the content liquid by utilizing the fact that the duration of the echo varies depending on whether or not the liquid is in contact with the inner wall surface.

[発明が解決しようとする課題] しかしながら、前記第1公報のものでは、容器内液面の
単一レベルしか検知することができず、限界上液面計な
いしは限界下液面計としてしか使用できない。
[Problems to be Solved by the Invention] However, in the above-mentioned first publication, only a single level of the liquid level in the container can be detected, and it can be used only as an upper limit liquid level gauge or a lower limit liquid level gauge. .

第2公報によるものでは、液面計を固定的に取り付ける
限りでは、上記第1公報のものと同様に連続的に変化す
る液面を当該レベルで検出することはできず、液面レベ
ルの上限また下限を検出する限界液面計であることにか
わりはない。
In the second publication, as long as the liquid level gauge is fixedly mounted, it is not possible to detect the continuously changing liquid surface at the level as in the first publication, and the upper limit of the liquid level is set. There is no change in that it is a limit level gauge that detects the lower limit.

また、前記液面計を壁面に沿って上下に移動させること
により、現在の液面レベルを検知することは可能である
が、液面計を一々移動させることは面倒であり、外壁面
の任意の場所において超音波の壁面に対する透過率を常
に一様に保つことの原理的な困難性を別としても、容器
が大型であったり、近接しにくい場所に設置されている
ような場合には、壁面に沿っての液面計の移動は一層困
難となり、実際上はやはり限界液面計として、その適用
範囲が限定されたものとなることは免れないところであ
る。
Further, it is possible to detect the current liquid level by moving the liquid level gauge up and down along the wall surface, but it is troublesome to move the liquid level gauge one by one, and it is not possible to move the liquid level gauge one by one. Aside from the principle difficulty of always maintaining the transmittance of the ultrasonic waves to the wall surface at the location of, even if the container is large or installed in a place where it is difficult to approach, The movement of the liquid level gauge along the wall surface becomes even more difficult, and in practice, it is unavoidable that the applicable range is limited as a limit level gauge.

上記問題点に関しては、さらに第3公報によるものに就
いても全く同様であり、前2者においては容器の内壁間
の透過音波ないしは反射音波であったのに対して、容器
殻壁内の多重反射波であることの相違だけである。
Regarding the above-mentioned problems, the same is true of the third publication. In the former two cases, the transmitted sound wave or the reflected sound wave between the inner walls of the container is different from the multiple sound wave inside the container shell wall. The only difference is that it is a reflected wave.

[発明の目的] 本発明は、このような従来の技術における問題点に鑑み
て成されたもので、一点の媒体の界面レベルだけでな
く、しかも受波器を移動させることなく容器内の複数の
媒体界面レベルに対応して検出可能な超音波界面レベル
計を提供することを目的としている。
[Object of the Invention] The present invention has been made in view of the above problems in the conventional technique, and is not limited to a single interface level of a medium, and a plurality of containers in a container can be formed without moving the wave receiver. It is an object of the present invention to provide an ultrasonic interface level meter that can detect the interface level of the medium.

[課題を解決するための手段] 上記目的を達成するためのこの発明の要旨とするところ
は、 (1)容器内の媒体検出面の測定域を挟んで超音波界面
レベル計の送波器と受波器とを配設し、 前記送波器からの超音波信号を所定周期のバースト波と
するとともに、 媒体に接する内壁面から媒体中へ超音波が漏洩するよう
に超音波を殻壁内へ入射させ、 殻壁と媒体中を通って容器内を往復する反射波の反射回
数を、媒体の界面レベルに対応した時間遅れ信号の数と
して受波器に入射させるようにしたことを特徴とする超
音波界面レベル計。
[Means for Solving the Problems] The gist of the present invention for achieving the above-mentioned object is as follows: (1) A transmitter of an ultrasonic interface level meter with a measurement area of a medium detection surface in a container being sandwiched therebetween. A wave receiver is provided, and the ultrasonic signal from the wave transmitter is converted into a burst wave having a predetermined period, and the ultrasonic wave is radiated into the medium from the inner wall surface in contact with the medium into the shell wall. It is characterized in that the number of reflections of reflected waves traveling back and forth inside the container through the shell wall and the medium is made to be incident on the receiver as the number of time-delayed signals corresponding to the interface level of the medium. Ultrasonic interface level meter.

(2)容器内の媒体検出面の測定域を挟んで超音波液面
計の送波器と受波器とを配設し、 前記送波器からの超音波信号を所定周期のバースト波と
するとともに、 媒体に接する内壁面から媒体中への超音波の漏洩が極大
値をとる下記条件式、 2d・cosθ=mλ (m=0、1、2・・・) 但し、dは殻壁の板厚、θは殻壁内に入射された超音
波の傾斜角、λは殻壁内の超音波の波長 を満足するようなθおよび/またはλによって超音
波を入射させ、 殻壁と媒体中を通って容器内を往復する反射波の反射回
数を、媒体の界面レベルに対応した時間遅れ信号の数と
して受波器に入射させるようにしたことを特徴とする請
求項1記載の超音波界面レベル計に存する。
(2) A wave transmitter and a wave receiver of an ultrasonic liquid level gauge are arranged across a measurement area of a medium detection surface in a container, and an ultrasonic signal from the wave transmitter is converted into a burst wave having a predetermined cycle. In addition, 2d · cos θ 1 = mλ 1 (m = 0,1,2 ...) where the ultrasonic wave leaks into the medium from the inner wall surface in contact with the medium is a maximum value, where d is a shell The plate thickness of the wall, θ 1 is the inclination angle of the ultrasonic wave incident on the shell wall, λ 1 is the ultrasonic wave incident on θ 1 and / or λ 1 that satisfies the wavelength of the ultrasonic wave inside the shell wall. The number of reflections of the reflected wave traveling back and forth inside the container through the shell wall and the medium is made incident on the receiver as the number of time-delayed signals corresponding to the interface level of the medium. It exists in the ultrasonic interface level meter described in 1.

[作用] 界面レベル計の送波器と受波器とを媒体容器において、
媒体の予想変動域を挟んで取り付ける。この際、送波器
と受波器の何れを上に、何れを下にしてもよい。
[Operation] In the medium container, the transmitter and the receiver of the interface level meter are
Install with the expected fluctuation range of the medium sandwiched. At this time, either the wave transmitter or the wave receiver may be on the upper side and any of the wave receiver may be on the lower side.

送波器から容器殻壁内に放射された超音波は、受波器と
の最短距離を伝わる伝達波のほかに、殻壁内の迂回経路
を通って到達した音波が重畳するので、連続波では意味
のある音波を弁別するのが難しい。そこで、一定の周期
と幅とを有するバースト波を放射する。
The ultrasonic wave radiated from the wave transmitter into the vessel shell wall is a continuous wave because not only the transmitted wave that travels the shortest distance from the wave receiver but also the acoustic wave that has reached through the detour path inside the shell wall are superposed. It is difficult to distinguish meaningful sound waves. Therefore, a burst wave having a constant period and width is radiated.

殻壁内面が媒体に接していないときには、固体である容
器と空気の固有音響インピーダンスの隔絶した相違か
ら、殻壁内に放射された超音波信号は、内壁面からは殆
ど容器内空中に拡散することなく、殻壁内の多重反射波
として伝搬していく。そして、媒体に接した所に達する
と、今度は容器の固有音響インピーダンスと媒体の固有
音響インピーダンスとは接近していて、超音波信号は内
壁面から媒体中に透過していく。送波器から放射される
信号超音波は内壁面から媒体への超音波の漏洩が極大値
をとる条件式、 2d・cosθ=mλ (m=0、1、2・・・) 但し、dは殻壁の板厚、θは殻壁内 の超音波の傾斜角、λは殻壁内の超音波の波長 を満足するようなθおよび/又はλに成っているか
ら、媒体に接した内壁面からは効率良く超音波の媒体中
への漏洩放射がなされる。
When the inner surface of the shell wall is not in contact with the medium, the ultrasonic signal radiated into the shell wall almost diffuses into the air inside the container due to the isolated difference in the intrinsic acoustic impedance between the solid container and air. Instead, it propagates as multiple reflected waves in the shell wall. Then, when it reaches a place in contact with the medium, the characteristic acoustic impedance of the container and the characteristic acoustic impedance of the medium are close to each other, and the ultrasonic signal is transmitted through the inner wall surface into the medium. The signal ultrasonic wave radiated from the wave transmitter has a conditional expression that the leakage of the ultrasonic wave from the inner wall surface to the medium has a maximum value, 2d · cos θ 1 = mλ 1 (m = 0, 1, 2, ...) d is the thickness of the shell wall, θ 1 is the inclination angle of the ultrasonic wave in the shell wall, and λ 1 is θ 1 and / or λ 1 that satisfies the wavelength of the ultrasonic wave in the shell wall. From the inner wall surface in contact with the medium, ultrasonic waves are efficiently radiated and leaked into the medium.

しかして、送波器から放射された超音波信号が媒体に接
している内壁面から漏洩し、漏洩超音波は対面する内壁
面から再度殻壁内に入り、外壁面で反射して殻壁内を通
り、再び媒体に漏洩していく。このような反射を繰り返
し、媒体に到達すると、以後は殻壁内の多重反射波とし
て受波器に入射する。送波器が媒体よりも上方にある場
合には、最初に殻壁内の多重反射として、そして媒体の
界面レベル以下では、媒体を通過する壁面間反射波とし
て受波器に入る。
Then, the ultrasonic signal radiated from the transmitter leaks from the inner wall surface in contact with the medium, the leaked ultrasonic wave enters the shell wall again from the facing inner wall surface, is reflected by the outer wall surface, and is reflected inside the shell wall. It passes through and leaks again to the medium. When such reflection is repeated and reaches the medium, it is subsequently incident on the wave receiver as multiple reflected waves in the shell wall. If the transmitter is above the medium, it enters the receiver first as multiple reflections in the shell wall and below the interface level of the medium as inter-wall reflected waves passing through the medium.

何れにしても、上記壁面間の反射波はその反射回数に対
応する時間遅れ信号として受波器に受信される。例え
ば、上記壁面間反射が3回であれば、殻壁内の伝達波の
信号を含めて4個のパルス波形が観測される。
In any case, the reflected wave between the wall surfaces is received by the wave receiver as a time delay signal corresponding to the number of reflections. For example, if the reflection between the wall surfaces is three times, four pulse waveforms including the signal of the transmitted wave in the shell wall are observed.

しかして、上記反射回数は媒体の界面レベルに対し段階
的に比例するから、この回数、すなわち受波器で得られ
る時間遅れパルスの数によって容器内の媒体の界面レベ
ルを知ることができる。
Since the number of reflections is stepwise proportional to the interface level of the medium, it is possible to know the interface level of the medium in the container by this number of times, that is, the number of time-delayed pulses obtained by the wave receiver.

[実施例] 次ぎに図面に基づき本発明を超音波計に適用した一実施
例について説明する。
[Embodiment] Next, an embodiment in which the present invention is applied to an ultrasonic meter will be described with reference to the drawings.

第1図に超音波液面計10の構成を示す。FIG. 1 shows the configuration of the ultrasonic level gauge 10.

超音波液面計(以下、単に液面計と称する。) 10は液体容器Vの下部に取り付けられた送波器11と、予
想液面を挟んだ上部に取り付けられた受波器12とからな
っている。(送波器11と受波器12の位置を反対にしても
よい。) 送波器11と受波器12とは同じ構造をなしており、第2図
(a)に外観図を、第2図(b)にその断面図を示して
いる。すなわち、ケーシング13に発信手段であるジルコ
ン酸・チタン酸鉛(PZT)の圧電素子14を、伝達媒体と
しての水中に固定して設けてある。そして容器Vに接す
る面には薄膜15が張ってある。もっとも、ケーシング13
を中実体とし、容器Vとの接触面に接着剤などで空気の
介在をなくするようにさえすれば、水などの媒介物は必
要としない。
An ultrasonic liquid level gauge (hereinafter, simply referred to as a liquid level gauge) 10 includes a wave transmitter 11 attached to a lower portion of a liquid container V and a wave receiver 12 attached to an upper portion with an expected liquid level in between. Has become. (The positions of the wave transmitter 11 and the wave receiver 12 may be reversed.) The wave transmitter 11 and the wave receiver 12 have the same structure, and an external view is shown in FIG. The sectional view is shown in FIG. That is, a piezoelectric element 14 made of zirconate / lead titanate (PZT), which is a transmitting means, is fixedly provided in the casing 13 in water as a transmission medium. A thin film 15 is stretched on the surface in contact with the container V. However, casing 13
Is a solid body, and a medium such as water is not required as long as air is not present on the contact surface with the container V with an adhesive or the like.

送波器11には指向特性と周波数特性によって入射角と周
波数の関係を満足させる事ができる圧電素子14の使用周
波数を発振する高周波発振手段例えば電圧制御発振器VC
Oなどとともに、この高周波をパルス変調するためのパ
ルス発生手段とを有する例えばパルスジェネレータ16が
結合されている。そして送波器11からは使用周波数のキ
ャリヤのパルス変調波(バースト波)が超音波信号とし
て発信される。
The wave transmitter 11 includes a high frequency oscillating means for oscillating the working frequency of the piezoelectric element 14 capable of satisfying the relationship between the incident angle and the frequency depending on the directional characteristic and the frequency characteristic, for example, the voltage controlled oscillator VC
For example, a pulse generator 16 having a pulse generating means for pulse-modulating this high frequency is coupled with O and the like. Then, from the wave transmitter 11, a pulse-modulated wave (burst wave) of a carrier having a used frequency is transmitted as an ultrasonic signal.

一方の受波器12には、受信信号を増幅する増幅器17と、
入力信号を処理するためのカウンタ、コンパレータなど
を含む信号処理回路と、処理結果として得られた液面レ
ベルを表示する表示手段とを備えた信号処理・表示装置
18が備えられている。
One of the wave receivers 12 has an amplifier 17 for amplifying the received signal,
A signal processing / display device including a signal processing circuit including a counter for processing an input signal, a comparator, and the like, and display means for displaying a liquid level obtained as a processing result.
Eighteen are equipped.

いま、第3図(a),(b)のように送波器の密度(g/
cm3)、音速(m/s)および入射角度(rad)を(ρ,C
,θ)、容器壁の密度(g/cm3)、音速(m/s)および
入射角度(rad)を(ρ、C,θ)、液中の密度
(g/cm3)、音速(m/s)および入射角度(rad)を(ρ
,C,θ)とし、容器壁の厚さをd(m)、入射し
た超音波の容器壁中の波長をλ(m)とする。ただし
θは全反射しない角度とする。
Now, as shown in FIGS. 3 (a) and 3 (b), the density (g /
cm 3 ), sound velocity (m / s) and incident angle (rad) as (ρ 0 , C
0 , θ), container wall density (g / cm 3 ), sound velocity (m / s) and incident angle (rad) (ρ 1 , C 1 , θ 1 ), density in liquid (g / cm 3 ) , Sound velocity (m / s) and incident angle (rad) (ρ
2 , C 2 , θ 2 ), the thickness of the container wall is d (m), and the wavelength of the incident ultrasonic wave in the container wall is λ 1 (m). However, θ is an angle at which total reflection does not occur.

ここで縦波のみを扱うと、これは三層の液体中へ超音波
を斜め入射した場合と同様になるので、送波器から液中
への超音波の透過率DはBoyleとRswlinsonによって次式
のように示されることがわかっている。
If only the longitudinal wave is treated here, this is the same as the case where the ultrasonic wave is obliquely incident into the liquid of three layers, so the transmittance D of the ultrasonic wave from the transmitter to the liquid is calculated by Boyle and Rswlinson as follows. It is known to be expressed as a formula.

しかして、上記透過率Dが極大値をもつ条件式はBoyle
とRawlinsonにより計算により導かれており、 2dcosθ=mλ (m=0,1,2,3,・・・) ・・・ となる。
Then, the conditional expression in which the transmittance D has a maximum value is Boyle
And Rawlinson, and it is 2dcosθ 1 = mλ 1 (m = 0,1,2,3, ...).

現実には入射されている超音波は縦波のみではなく、ま
た、送波器や受波器の特性や介在物などにより透過率D
は式の通りにはならない。しかし、極大値を持つ条件
式式は縦波には成り立っているので縦波のみを扱うよ
うにすれば極大値を持つ条件式式より、容器壁の厚さ
dが与えられたとき、式をみたすようにθおよび/
又はλを与えることにより、液面レベルの変化に鋭く
反応する液面計とすることができる。
In reality, the incident ultrasonic waves are not only longitudinal waves but also the transmittance D due to the characteristics of the transmitter and the receiver and inclusions.
Does not follow the formula. However, since the conditional expression having the maximum value is valid for the longitudinal wave, if only the longitudinal wave is treated, the conditional expression having the maximum value gives the expression when the thickness d of the container wall is given. As you can see, θ 1 and /
Alternatively, by providing λ 1 , it is possible to obtain a liquid level meter that reacts sharply to changes in the liquid level.

そこで、例えば第4図(a)のように液面レベルが非常
に低い場合には、送波器11から放射された信号超音波は
効率良く液中に漏洩するが、対面する容器壁面に到達す
る前に液表面に到達し、その入射角および液体と空気と
の固有音響インピーダンスの相違から空中への漏洩はな
く、反射して容器内を複雑に反射、漏洩を繰り返して減
衰していく。そして、伝達波だけが受波器12に受信され
る。
Therefore, for example, when the liquid level is very low as shown in FIG. 4 (a), the signal ultrasonic waves emitted from the wave transmitter 11 efficiently leak into the liquid, but reach the wall surface of the facing container. Before reaching the liquid surface, there is no leakage into the air due to the difference in the incident angle and the inherent acoustic impedance between the liquid and air, and the light is reflected and reflected intricately inside the container, and the leakage is repeatedly attenuated. Then, only the transmitted wave is received by the wave receiver 12.

以下、第4図(a)〜第5図(d)によって作用を説明
する。
The operation will be described below with reference to FIGS. 4 (a) to 5 (d).

上にも述べたように、液面レベルが低いときには、受波
器12には第5図(a)に示すように伝達波信号a0だけが
受信され、漏洩も殆どなく、信号レベル自体も減衰の少
ないものである。
As described above, when the liquid level is low, the receiver 12 receives only the transmitted wave signal a 0 as shown in FIG. It has little attenuation.

第4図(b)のように液体がやや多いときには、液中に
漏洩した信号波は対面する容器壁面から殻壁内に透過
し、外壁面で反射して再び液中に戻り、こちら側の外壁
面で反射して再々度液中に漏洩するが、対面する壁面に
到達できず、有効な反射波は1回だけで、第5図(b)
に示すように伝達波信号a0のほかには1個だけの反射波
信号a1が遅延パルスとして観測される。
When the liquid is a little large as shown in FIG. 4 (b), the signal wave leaking into the liquid is transmitted from the facing wall surface of the container to the inside of the shell wall, is reflected by the outer wall surface, and returns to the liquid again. Although it is reflected on the outer wall surface and leaks again into the liquid, it cannot reach the facing wall surface, and the effective reflected wave is only once.
As shown in FIG. 5, only one reflected wave signal a 1 is observed as a delayed pulse in addition to the transmitted wave signal a 0 .

第4図(c)のようにさらに液面が高いと反射波は第5
図(c)のように時間遅れ信号a1、a2と2個得られる。
If the liquid surface is higher as shown in FIG.
As shown in FIG. 7C, two time delay signals a 1 and a 2 are obtained.

第4図(d)では高い液面レベルで第5図(d)のよう
に3個の反射波信号a1、a2、a3が得られる場合を示して
いる。
FIG. 4 (d) shows a case where three reflected wave signals a 1 , a 2 and a 3 are obtained at a high liquid level as shown in FIG. 5 (d).

第5図各図に見るように、反射波が多くなると、伝達波
など先に受信される信号は漏洩が多くなって信号レベル
が低下している。
As shown in each of FIG. 5, when the reflected wave increases, the signal received earlier such as the transmitted wave leaks more and the signal level decreases.

なお、本実施例では送波器11を下部に、受波器12を容器
Vの測定域を挟んだ上部に取り付けたが、これとは逆の
取り付け方であってもよい。
In the present embodiment, the wave transmitter 11 is attached to the lower portion and the wave receiver 12 is attached to the upper portion of the container V with the measurement region sandwiched between them. However, the attachment method may be reversed.

本発明の超音波液面計10では、液体に接する壁面が長
く、また液体の固有音響インピーダンスが大きくて液中
への漏洩が多くなり、直達波の信号レベルが小さくなる
場合でも液面レベルに関する情報を確実に得ることがで
きる。
In the ultrasonic liquid level meter 10 of the present invention, the wall surface in contact with the liquid is long, and the liquid has a large specific acoustic impedance, so that leakage into the liquid is increased, and the signal level of the direct wave is reduced. Information can be surely obtained.

[発明の効果] 本発明は、検出媒体の測定域を挟んで送波器と受波器と
を取り付け、送波器からの発信信号を所定周期のバース
ト波とするとともに、媒体に接する内壁面から液中へ超
音波が漏洩するように超音波を入射させ、殻壁と媒体中
を通って容器内を往復する反射波の反射回数を、媒体の
界面レベルに対応した遅延信号の数として受波器に入射
させるようにしたから、固有音響インピーダンスの大き
い媒体で、しかも媒体界面レベルが高く、漏洩波が多く
なって伝達波信号レベルが微小になるような場合でも、
媒体界面レベルに関する情報を確実に得ることができ、
送波器や受波器を移動させることなく、容器内の複数の
媒体界面レベルを検出することが可能となった。
[Advantages of the Invention] The present invention has a wave transmitter and a wave receiver attached across a measurement area of a detection medium, makes a transmission signal from the wave transmitter a burst wave of a predetermined period, and also has an inner wall surface in contact with the medium. The ultrasonic wave is made incident so that it leaks from the liquid into the liquid, and the number of reflections of the reflected wave traveling back and forth inside the container through the shell wall and the medium is received as the number of delayed signals corresponding to the interface level of the medium. Since it is made incident on the wave device, even in the case where the medium has a large specific acoustic impedance, and the medium interface level is high and the number of leaked waves is large and the transmitted wave signal level becomes minute,
You can certainly get information about the media interface level,
It has become possible to detect multiple media interface levels in a container without moving the transmitter and receiver.

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

第1図〜第5図(d)は本発明の一実施例を示してお
り、第1図は全体の構成図、第2図(a)は送波器、受
波器の外観図、第2図(b)は同じく断面図、第3図は
漏洩原理の説明図、第4図(a)〜第4図(d)は液面
レベルと反射波の個数の関係をしめす作用説明図、第5
図(a)〜第5図(d)はそれぞれ第4図(a)〜第4
図(d)に対応した反射波信号の作用説明図である。 10……超音波液面計 11……送波器 12……受波器 13……ケーシング 14……圧電素子 16……パルスジェネレータ 17……増幅器 18……信号処理・表示装置 V……液体容器 a0……直達波 a1……1回反射波信号 a2……2回反射波信号 a3……3回反射波信号
1 to 5 (d) show an embodiment of the present invention, FIG. 1 is an overall configuration diagram, and FIG. 2 (a) is an external view of a transmitter and a receiver. 2 (b) is a sectional view of the same, FIG. 3 is an explanatory diagram of the principle of leakage, and FIGS. 4 (a) to 4 (d) are explanatory diagrams of the action showing the relationship between the liquid surface level and the number of reflected waves. Fifth
FIGS. 4 (a) to 5 (d) are shown in FIGS. 4 (a) to 4 respectively.
It is an action explanatory view of a reflected wave signal corresponding to Drawing (d). 10 …… Ultrasonic liquid level gauge 11 …… Transmitter 12 …… Receiver 13 …… Casing 14 …… Piezoelectric element 16 …… Pulse generator 17 …… Amplifier 18 …… Signal processing / display device V …… Liquid Container a 0 …… Direct wave a 1 …… One-time reflected wave signal a 2 …… Two-time reflected wave signal a 3 …… Three-time reflected wave signal

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】容器内の媒体検出面の測定域を挟んで超音
波界面レベル計の送波器と受波器とを配設し、 前記送波器からの超音波信号を所定周期のバースト波と
するとともに、 媒体に接する内壁面から媒体中へ超音波が漏洩するよう
に超音波を殻壁内へ入射させ、 殻壁と媒体中を通って容器内を往復する反射波の反射回
数を、媒体の界面レベルに対応した時間遅れ信号の数と
して受波器に入射させるようにしたことを特徴とする超
音波界面レベル計。
1. A wave transmitter and a wave receiver of an ultrasonic interface level meter are arranged across a measurement area of a medium detection surface in a container, and an ultrasonic signal from the wave transmitter is burst in a predetermined cycle. The ultrasonic wave is made to enter the shell wall so that the ultrasonic wave leaks into the medium from the inner wall surface in contact with the medium, and the number of reflections of the reflected wave traveling back and forth inside the container through the shell wall and the medium is reflected. The ultrasonic interface level meter is characterized in that the number of time-delayed signals corresponding to the interface level of the medium is made incident on the wave receiver.
【請求項2】容器内の媒体検出面の測定域を挟んで超音
波液面計の送波器と受波器とを配設し、 前記送波器からの超音波信号を所定周期のバースト波と
するとともに、 媒体に接する内壁面から媒体中への超音波の漏洩が極大
値をとる下記条件式、 2d・cosθ=mλ (m=0、1、2・・・) 但し、dは殻壁の板厚、θは殻壁内に入射された超音
波の傾斜角、λは殻壁内の超音波の波長 を満足するようなθおよび/又はλによって超音波
を入射させ、 殻壁と媒体中を通って容器内を往復する反射波の反射回
数を、媒体の界面レベルに対応した時間遅れ信号の数と
して受波器に入射させるようにしたことを特徴とする請
求項1記載の超音波界面レベル計。
2. A wave transmitter and a wave receiver of an ultrasonic liquid level gauge are arranged across a measurement area of a medium detection surface in a container, and an ultrasonic signal from the wave transmitter is burst in a predetermined cycle. Waveform and the following conditional expression in which the leakage of ultrasonic waves from the inner wall surface in contact with the medium to the medium has a maximum value, 2d · cos θ 1 = mλ 1 (m = 0, 1, 2, ...) where d Is the thickness of the shell wall, θ 1 is the inclination angle of the ultrasonic wave incident into the shell wall, and λ 1 is the ultrasonic wave with θ 1 and / or λ 1 that satisfies the wavelength of the ultrasonic wave in the shell wall. It is characterized in that the number of reflections of reflected waves that are made incident and travel back and forth inside the container through the shell wall and the medium is made incident on the receiver as the number of time-delayed signals corresponding to the interface level of the medium. The ultrasonic interface level meter according to claim 1.
JP2319537A 1990-11-21 1990-11-21 Ultrasonic interface level meter Expired - Lifetime JPH0778445B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2319537A JPH0778445B2 (en) 1990-11-21 1990-11-21 Ultrasonic interface level meter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2319537A JPH0778445B2 (en) 1990-11-21 1990-11-21 Ultrasonic interface level meter

Publications (2)

Publication Number Publication Date
JPH04188028A JPH04188028A (en) 1992-07-06
JPH0778445B2 true JPH0778445B2 (en) 1995-08-23

Family

ID=18111354

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2319537A Expired - Lifetime JPH0778445B2 (en) 1990-11-21 1990-11-21 Ultrasonic interface level meter

Country Status (1)

Country Link
JP (1) JPH0778445B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2577417Y2 (en) * 1993-03-03 1998-07-30 三菱重工業株式会社 mechanical seal

Also Published As

Publication number Publication date
JPH04188028A (en) 1992-07-06

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