JPH0716977Y2 - Ultrasonic probe and ultrasonic flowmeter using the same - Google Patents

Ultrasonic probe and ultrasonic flowmeter using the same

Info

Publication number
JPH0716977Y2
JPH0716977Y2 JP4881991U JP4881991U JPH0716977Y2 JP H0716977 Y2 JPH0716977 Y2 JP H0716977Y2 JP 4881991 U JP4881991 U JP 4881991U JP 4881991 U JP4881991 U JP 4881991U JP H0716977 Y2 JPH0716977 Y2 JP H0716977Y2
Authority
JP
Japan
Prior art keywords
ultrasonic
vibrator
probe
ultrasonic probe
holder
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
JP4881991U
Other languages
Japanese (ja)
Other versions
JPH04134023U (en
Inventor
裕 柏瀬
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.)
Tokyo Keiki Inc
Original Assignee
Tokyo Keiki Inc
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 Keiki Inc filed Critical Tokyo Keiki Inc
Priority to JP4881991U priority Critical patent/JPH0716977Y2/en
Publication of JPH04134023U publication Critical patent/JPH04134023U/en
Application granted granted Critical
Publication of JPH0716977Y2 publication Critical patent/JPH0716977Y2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Description

【考案の詳細な説明】[Detailed description of the device]

【0001】[0001]

【産業上の利用分野】本考案は、超音波プローブ及びそ
れを用いた超音波流量計に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an ultrasonic probe and an ultrasonic flowmeter using the ultrasonic probe.

【0002】[0002]

【従来の技術】従来、超音波を利用した計測装置として
は、超音波量計及び超音波距離等が一般に広く知られて
いる。これらの計測装置は、その計測手段として、超音
波を超音波プローブから送受信して、これらの伝播時間
の差を基にして演算を行ない測定値を表示するものと成
っている。
2. Description of the Related Art Conventionally, as a measuring device using ultrasonic waves, an ultrasonic quantity meter and an ultrasonic distance are widely known. As a measuring means of these measuring devices, ultrasonic waves are transmitted and received from an ultrasonic probe, and calculation is performed based on the difference in their propagation times to display measured values.

【0003】図6に従来より知られている超音波流量計
を示す。この図6において、符号20は被測定物質を通
過させる測定管を示し、符合21及び符号22はそれぞ
れ超音波を授受する超音波プローブを示す。また符号2
3及び符号24は超音波プローブ21,22を装着する
筒体である。超音波プローブ21,22は、筒体23,
24とによって測定管20の軸線上にそれぞれ向けて所
定傾斜角度θをもって装着されている。
FIG. 6 shows a conventionally known ultrasonic flowmeter. In FIG. 6, reference numeral 20 indicates a measuring tube through which the substance to be measured passes, and reference numerals 21 and 22 indicate ultrasonic probes for transmitting and receiving ultrasonic waves, respectively. Also reference numeral 2
Reference numeral 3 and reference numeral 24 are cylindrical bodies on which the ultrasonic probes 21 and 22 are mounted. The ultrasonic probes 21 and 22 have a cylindrical body 23,
And 24 are mounted at a predetermined inclination angle θ toward the axis of the measuring tube 20, respectively.

【0004】配管内の流量測定は、配管20の内に被測
定物に対し、ブローブ21,22の間で超音波パルスを
A,B方向に交互に繰り返して送受信し、それぞれ発信
する超音波パルスの方向と被測定物質の流れる方向に対
して、順方向の伝播時間と、逆方向の伝播時間を測定す
ることにより行なわれる。そして、それぞれの伝播時間
の差から被測定物の流速Vを求め、さらに配管20の断
面積を用いることにより、単位時間当たりの流量が算定
される。
The flow rate in the pipe is measured by alternately transmitting and receiving ultrasonic pulses in the A and B directions between the probes 21 and 22 with respect to the object to be measured in the pipe 20 and transmitting ultrasonic pulses. The measurement is performed by measuring the forward propagation time and the backward propagation time with respect to the direction and the flowing direction of the substance to be measured. Then, the flow rate V per unit time is calculated by obtaining the flow velocity V of the measured object from the difference between the respective propagation times and further using the cross-sectional area of the pipe 20.

【0005】[0005]

【考案が解決しようとする課題】しかしながら、かかる
従来の超音波流量計おいて、図7に示すように超音波プ
ローブ21、22から発信された超音波パルスは、本来
の伝播経路A,Bの他に、超音波プローブ21,22の
取付け接触部分25,26から配管20の管壁中等を伝
って伝播する伝播経路a,bが存在する。ここで、本来
の伝播経路A,Bにおける超音波の伝播速度は被測定物
が空気の場合で約350[m/S]であるのに対し、伝
播経路a,bにおける伝播速度は配管が鋼管の場合で約
5000[m/S]である。これらの音速の差は、超音
波の通る媒体によって固有の超音波の伝播速度を有して
いるため生ずるものであり、経路a,bを伝播してくる
パルス波の方が、本来の経路A,Bを伝播してくるパル
ス波より早く受信側の超音波プローブに到達するという
現象が生じてしまう。また、この経路a,bを伝播する
パルス波は、複数の経路が存在する上に、複数の部品の
中を伝播していくため、部品同士の接触部の境界におけ
る反射や、この残響が重畳される。このため、著しく長
い尾を引いたパルスとなり、本来情報として欲しい経路
Aのパルス波と重なる。このため、この受信波の検出
が、困難になるという不都合があった。さらに、伝播時
間の測定誤差を生じ、従って流量測定そのものの精度も
著しく低下するという不都合があった。
However, in such a conventional ultrasonic flowmeter, as shown in FIG. 7, the ultrasonic pulses emitted from the ultrasonic probes 21 and 22 have the original propagation paths A and B. In addition, there are propagation paths a and b which propagate from the attachment contact portions 25 and 26 of the ultrasonic probes 21 and 22 through the pipe wall of the pipe 20 and the like. Here, the propagation speed of the ultrasonic waves in the original propagation paths A and B is about 350 [m / S] when the object to be measured is air, whereas the propagation speed in the propagation paths a and b is steel pipes. In the case of, it is about 5000 [m / S]. The difference between these sound velocities occurs because the medium through which the ultrasonic waves pass has an inherent ultrasonic wave propagation velocity, and the pulse wave propagating through the paths a and b is the original path A. , B arrives at the ultrasonic probe on the receiving side earlier than the pulse wave propagating in B. Further, since the pulse waves propagating through the paths a and b have a plurality of paths and propagate through a plurality of parts, reflection at the boundary between the contact parts of the parts and this reverberation are superimposed. To be done. For this reason, the pulse has a remarkably long tail, and overlaps with the pulse wave of the route A that is originally desired as information. Therefore, there is an inconvenience that it is difficult to detect the received wave. Further, there is a disadvantage that a measurement error of the propagation time is generated, and thus the accuracy of the flow rate measurement itself is significantly reduced.

【0006】図8にこれら従来例における各状態の受信
波形を示す。図8(a)は経路Aを伝播する本来の受信
波、(b)は測定管を伝播する妨害波を示す。一般に伝
播時間の測定はゼロクロス点において行うため、その点
の拡大図を同図(c)および(d)に示す。本来の受信
波(実線)と妨害波(点線)の位相関係は、伝播経路
長,伝播媒体の音速,被測定流体の流速等の条件によっ
て変化するため、種々条件が考えられるが、ゼロクロス
点における妨害波がプラス(+)の最大値になる場合を
(c)、妨害波がマイナス(−)の最大値になる場合を
(d)に示す。この場合、(c)では、時間軸に対して
本来の受信時刻tよも測定点t’が遅くなり、同図右方
にずれる。また(d)では、時間軸に対して本来の受信
時刻tよりも測定点t’が早くなり、同図左方にずれ
る。これらの結果として図9に示すように、正規の受信
波の他に妨害波が重畳され、このため、伝播時間の測定
が不正確になり測定精度が低下する、という不都合があ
った。一方、同様の事態が、他の計測装置、例えば送受
信プローブを別々に装備した反射形の超音波距離測定装
置においても生じていた。
FIG. 8 shows received waveforms in each state in these conventional examples. FIG. 8A shows an original received wave propagating along the path A, and FIG. 8B shows an interfering wave propagating through the measuring tube. In general, the propagation time is measured at the zero-cross point, so enlarged views of that point are shown in FIGS. The phase relationship between the original received wave (solid line) and the interfering wave (dotted line) changes depending on conditions such as the propagation path length, the sound velocity of the propagation medium, and the flow velocity of the fluid to be measured. (C) shows the case where the interference wave has a maximum value of plus (+), and (d) shows the case where the interference wave has a maximum value of minus (-). In this case, in (c), the measurement point t'becomes later than the original reception time t with respect to the time axis, and is shifted to the right in the figure. Further, in (d), the measurement point t'becomes earlier than the original reception time t with respect to the time axis, and is shifted to the left in the figure. As a result of these, as shown in FIG. 9, an interfering wave is superposed on the normal received wave, which causes inconvenience in measuring the propagation time and lowering the measurement accuracy. On the other hand, the same situation has occurred in other measuring devices, for example, a reflection type ultrasonic distance measuring device equipped with a transmitting / receiving probe separately.

【0007】[0007]

【考案の目的】本考案の目的は、かかる従来例の有する
不都合を改善し、特に雑音の混入を有効に排除するとと
もに、測定精度の向上を図った超音波プローブ及びそれ
を用いた超音波流量計を提供することを、その目的とす
る。
SUMMARY OF THE INVENTION The object of the present invention is to improve the inconveniences of the conventional example, particularly to effectively eliminate the mixing of noise, and to improve the measurement accuracy, and an ultrasonic probe and an ultrasonic flow rate using the same. The purpose is to provide a total.

【0008】[0008]

【課題を解決するための手段】本考案では、超音波振動
子を一端部に装備した振動子保持体と、この振動子保持
体を支持する支持部材とを備えた超音波プローブを設
け、この超音波プローブが備えている振動子保持体と支
持部材との間に、吸振部材を介装する、という構成を採
っている。
According to the present invention, there is provided an ultrasonic probe having a vibrator holder having an ultrasonic vibrator at one end and a support member for supporting the vibrator holder. A configuration is adopted in which a vibration absorbing member is interposed between a vibrator holder and a supporting member included in the ultrasonic probe.

【0009】さらに、本考案では、配管を介して所定距
離を隔てて配設された流量測定用の一対の超音波プロー
ブと、この超音波プローブを配管の軸線に対して所定の
傾斜角をもって着脱自在に且つ密封状態に装備するプロ
ーブホルダとを備えている。そして、超音波プローブ
を、振動子保持体とこれを支持する支持部材とを有し且
つ当該振動子保持体と支持部材との間に吸振部材を備え
たものを使用する、という構成を採っている。これらに
よって前述した目的を達成しようとするものである。
Further, according to the present invention, a pair of ultrasonic probes for flow rate measurement, which are arranged at a predetermined distance through the pipe, and the ultrasonic probe are attached and detached at a predetermined inclination angle with respect to the axis of the pipe. And a probe holder that is freely and hermetically mounted. Then, an ultrasonic probe having a vibrator holder and a support member for supporting the vibrator and having a vibration absorbing member between the vibrator holder and the support member is used. There is. These are intended to achieve the above-mentioned object.

【0010】[0010]

【作用】超音波振動子が振動すると、その振動波(超音
波)は振動子保持体内にも伝播し、続いて支持部材側へ
伝播する状態となる。一方、この支持部材と振動子保持
体との間には吸収部材が介装されていることから、この
吸収部材の作用により支持部材側へ伝播する超音波成分
は有効に遮断される。
When the ultrasonic vibrator vibrates, the vibration wave (ultrasonic wave) propagates inside the vibrator holder and then propagates to the support member side. On the other hand, since the absorbing member is interposed between the supporting member and the oscillator holder, the ultrasonic component propagating to the supporting member side is effectively blocked by the action of the absorbing member.

【0011】[0011]

【第1実施例】以下、本考案の第1実施例を図1に基づ
いて説明する。この図1において、符号20は配管を示
し、符合21は超音波プローブ用のプローグホルダを示
す。このプローブホルダ21は、配管20の内壁に一端
部を開口した開口部27を有するとともに、この配管2
0の軸線上に、所定の傾斜角度をもってそれぞれに対向
して配設されている。
[First Embodiment] A first embodiment of the present invention will be described below with reference to FIG. In FIG. 1, reference numeral 20 indicates a pipe, and reference numeral 21 indicates a probe holder for an ultrasonic probe. The probe holder 21 has an opening 27 having one end opened on the inner wall of the pipe 20, and the pipe 2
They are arranged so as to face each other at a predetermined inclination angle on the axis 0.

【0012】一方、このプローブホルダ21には、振動
子保持部材1,支持部材2及び制御部8から成るプロー
ブ全体が装着されている。振動子保持部材1の配管20
側一端部には、超音波発振源となる振動子6が装着され
ており、またこの振動子保持部材1の中央部と他端部に
は、該振動子保持部材1の外径に沿って突出された鍔部
1a,1bがそれぞれ設けられいる。そして、この鍔部
1aと1bに囲まれた軸部1cの当該鍔部1aと1bと
が交わる角部に、弾性部材から成る平リング状のタンパ
ー5およびOリング3,4(吸振部材)がそれぞれ組み
込まれている。これらの吸振部材が組み込まれた軸部1
cは、筒状の支持部材2の内径部に貫入される。そし
て、この様に振動子保持部材1を装着した支持部材の鍔
部2aはプローブホルダ21の終端部へフクロナット3
0でネジ止めされるとともに、Oリング28によりシー
ルされる。また、超音波振動子6への信号の送受は、支
持部材2の終端部にネジ止め係止された制御部8から、
振動子保持部材1とを連結する(図示せず)ケーブルに
よって行われる。
On the other hand, the probe holder 21 is mounted with the entire probe including the vibrator holding member 1, the supporting member 2 and the control unit 8. Piping 20 of vibrator holding member 1
A vibrator 6 serving as an ultrasonic wave oscillation source is attached to one side end, and the center and the other end of the vibrator holding member 1 are arranged along the outer diameter of the vibrator holding member 1. Projected collar portions 1a and 1b are provided, respectively. Then, a flat ring-shaped tamper 5 made of an elastic member and O-rings 3 and 4 (vibration absorbing member) are provided at the corners of the shaft portion 1c surrounded by the flange portions 1a and 1b where the flange portions 1a and 1b intersect. Each is incorporated. Shaft part 1 incorporating these vibration absorbing members
The c is inserted into the inner diameter portion of the tubular support member 2. Then, the collar portion 2a of the supporting member having the vibrator holding member 1 mounted in this way is attached to the end portion of the probe holder 21 by the hook nut 3a.
It is screwed with 0 and sealed by the O-ring 28. Further, the transmission and reception of the signal to and from the ultrasonic transducer 6 is performed by the control unit 8 screwed and locked to the terminal end of the support member 2.
It is performed by a cable (not shown) connecting to the vibrator holding member 1.

【0013】この様な構成によって振動子保持部材1は
組み込まれているので、振動子保持部材1の軸部1c
は、適度に離れた長手方向に2箇所にOリング3,4を
介して支持部材2の内径部に間隙を持って保持されてい
る。このため、振動子保持部材1は軸線長手方向(超音
波振動子の振動方向)のみの自由度が生じる。また、振
動子保持部材の鍔部1aと支持部材2との長手方向での
接触点には、ダンパー5が装備されている。これによ
り、振動子保持部材1と支持部材2との絶縁が可能とな
っている。
Since the vibrator holding member 1 is incorporated by such a structure, the shaft portion 1c of the vibrator holding member 1 is assembled.
Are held in the inner diameter portion of the support member 2 with gaps at two positions in the longitudinal direction, which are appropriately separated, via O-rings 3 and 4. For this reason, the vibrator holding member 1 has a degree of freedom only in the longitudinal direction of the axis (the vibration direction of the ultrasonic vibrator). Further, a damper 5 is provided at a contact point between the flange portion 1a of the vibrator holding member and the support member 2 in the longitudinal direction. As a result, the vibrator holding member 1 and the support member 2 can be insulated.

【0014】次に、上記実施例の動作について説明す
る。図1において、超音波振動子6は、制御部8により
ケーブル(図示せず)を介して信号を受けるとともに超
音波振動を開始する。そして、これにより生じた超音波
9は、測定管の開口部27を通り被測定物中を通過す
る。そして、配管20の同軸上に所定の傾斜角度を持っ
て互いに対向する他方に配設された図1と同様の超音波
振動子(図示せず)との間で、この超音波の送受が行わ
れる。この時、超音波振動子6を保持する振動子保持部
材1も超音波振動子6とともに振動する。この超音波振
動は振動子保持部材1の軸線長手方向と同一の前後振動
であるので、振動子保持部材1は、保持部材中央部の軸
部1cを所定の間隔をもって長手方向に2箇所弾性部材
のOリング3,4を介して支持部材2の内径部に間隙を
持って保持されているため、軸線長手方向(超音波振動
方向)に従動した柔軟的な動きが行なえる。
Next, the operation of the above embodiment will be described. In FIG. 1, the ultrasonic vibrator 6 receives a signal from the control unit 8 via a cable (not shown) and starts ultrasonic vibration. Then, the ultrasonic wave 9 generated thereby passes through the measurement object through the opening 27 of the measuring tube. Then, the ultrasonic wave is transmitted and received between the ultrasonic transducer (not shown) similar to that shown in FIG. 1 which is arranged on the other side of the pipe 20 coaxially with each other with a predetermined inclination angle. Be seen. At this time, the vibrator holding member 1 that holds the ultrasonic vibrator 6 also vibrates together with the ultrasonic vibrator 6. Since this ultrasonic vibration is the same longitudinal vibration as the longitudinal direction of the axis of the vibrator holding member 1, the vibrator holding member 1 has two elastic members in the longitudinal direction with the shaft portion 1c at the center of the holding member at a predetermined interval. Since they are held with a gap in the inner diameter portion of the support member 2 through the O-rings 3 and 4, the flexible movement can be performed following the longitudinal direction of the axis (the ultrasonic vibration direction).

【0015】図5に従来例の場合と同一の条件で送受信
した場合の受信側で測定した受信波も測定結果を示す。
これによると妨害波部分が大幅に少なくなっていること
がわかる。
FIG. 5 also shows the measurement results of the received waves measured on the receiving side when transmitting and receiving under the same conditions as in the conventional example.
According to this, it can be seen that the disturbing wave portion is significantly reduced.

【0016】[0016]

【第2実施例】図2に第2実施例を示す。この図2に示
す第2実施例は、前述した振動子保持部材1の終端部を
延長して、制御部8のケース10と直接ネジ止め係止し
たものである。このため、振動子保持部材1とプローブ
ホルダ21とが配管20と直接接触している支持部材2
を介さずに接続されるので、配管20を伝播媒体とする
妨害波から振動子保持部材1に装着された超音波振動子
6を隔離することができる。なお、他の構成は、第1実
施例と同様のものと成っている。
[Second Embodiment] FIG. 2 shows a second embodiment. In the second embodiment shown in FIG. 2, the end portion of the vibrator holding member 1 described above is extended and directly screwed and locked to the case 10 of the control unit 8. Therefore, the support member 2 in which the vibrator holding member 1 and the probe holder 21 are in direct contact with the pipe 20
Therefore, the ultrasonic transducer 6 mounted on the transducer holding member 1 can be isolated from an interfering wave using the pipe 20 as a propagation medium. The other structure is similar to that of the first embodiment.

【0017】[0017]

【第3実施例】図3ないし図4に第3実施例を示す。こ
の図3ないし図4に示す第3実施例は、前述した振動子
保持部材1とこの保持部材1を貫入保持する支持部材2
との嵌合部に、合対向する軸線長手方向に溝部13,1
3a,14,14aを設けている。そして、この溝部に
は鋼球11,11a,12,12aをそれぞれ配設した
構成となっている。このため、支持部材との間隙部にリ
ニアベアリング状の摺動機構部を設けた振動子保持部材
1は、軸線長手方向(超音波振動方向)に対して自由に
従動した動きが行なえる。一方、この振動子保持部材1
の終端部には空間部7を通して、弾性部材等から成るス
プリング13を装着することにより、上述した振動子保
持部材1の軸線長手方向(超音波振動方向)の動きに対
応した柔軟的な動きが行なわれている。
[Third Embodiment] FIGS. 3 to 4 show a third embodiment. In the third embodiment shown in FIGS. 3 to 4, the vibrator holding member 1 and the supporting member 2 for holding the vibrator holding member 1 in a penetrating manner are provided.
To the mating portion with the groove portions 1
3a, 14, 14a are provided. Then, steel balls 11, 11a, 12, 12a are arranged in the groove portions, respectively. Therefore, the vibrator holding member 1 provided with the linear bearing-shaped sliding mechanism portion in the gap with the support member can freely follow the axial longitudinal direction (ultrasonic vibration direction). On the other hand, this vibrator holding member 1
By mounting the spring 13 made of an elastic member or the like through the space 7 at the end portion of the, a flexible movement corresponding to the movement of the vibrator holding member 1 in the longitudinal direction of the axis (ultrasonic vibration direction) can be achieved. Has been done.

【0018】ここで、上述した各実施例では、超音波プ
ローブを超音波流量計について本考案を実施した場合の
実施例であるが、この超音波プローブは超音波距離計等
について実施したものであってもよい。
In each of the above-mentioned embodiments, the ultrasonic probe is an ultrasonic flowmeter, and the ultrasonic probe is an ultrasonic rangefinder. It may be.

【0019】[0019]

【考案の効果】本考案は以上のように構成され機能する
ので、これによると、超音波振動子とともに共振する振
動子保持部材の振動を支持部材から外部への伝達を防止
できるため、送信時に超音波プローブと接触した配管へ
超音波振動の伝播を有効に遮断することができ、受信時
には配管壁内を伝播してくる妨害波を超音波プローブ部
分で遮断できる。このため、妨害波が重畳されることが
防止されることとなる。このため、流量測定にあって
は、ノイズの同時受信を有効に防止することができ、従
って、妨害波の重畳されない安定した精度の高い流量測
定が可能になる。また、プローブホルダ内部に装着され
た超音波プローブとの間隙に、ダスト等が堆積すること
によってホルダ内部と超音波プローブとの間に音響的カ
ップリングが生じた場合においても、超音波プローブの
振動子保持部材は外部との絶縁が保たれるため、妨害波
の影響を防ぐことが可能となり、かかる点においても精
度を著しく向上させることができるという従来例にない
実用的な超音波プローブ及びそれを用いた超音波流量計
を提供できる。
Since the present invention is constructed and functions as described above, it is possible to prevent the vibration of the vibrator holding member, which resonates together with the ultrasonic vibrator, from being transmitted from the support member to the outside. It is possible to effectively block the propagation of ultrasonic vibrations to the pipe in contact with the ultrasonic probe, and to block the interfering wave propagating inside the pipe wall at the time of reception by the ultrasonic probe portion. Therefore, it is possible to prevent the interference wave from being superimposed. Therefore, in the flow rate measurement, simultaneous reception of noise can be effectively prevented, and thus stable and highly accurate flow rate measurement in which no interfering wave is superimposed can be performed. In addition, even when acoustic coupling occurs between the inside of the holder and the ultrasonic probe due to the accumulation of dust or the like in the gap between the ultrasonic probe mounted inside the probe holder, the vibration of the ultrasonic probe Since the child holding member is kept insulated from the outside, it is possible to prevent the influence of interfering waves, and also in this respect, it is possible to remarkably improve the accuracy, and a practical ultrasonic probe and an unprecedented practical ultrasonic probe. An ultrasonic flowmeter using the can be provided.

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

【図1】本考案の第1実施例を示す横断面図FIG. 1 is a cross sectional view showing a first embodiment of the present invention.

【図2】第2実施例を示す横断面図FIG. 2 is a cross sectional view showing a second embodiment.

【図3】第3実施例を示す縦断面図FIG. 3 is a vertical sectional view showing a third embodiment.

【図4】図3内のA−A’線に沿った断面図4 is a cross-sectional view taken along the line A-A ′ in FIG.

【図5】図1の実施例における受信波の状態を示す線図5 is a diagram showing a state of a received wave in the embodiment of FIG.

【図6ないし図7】従来例を示す一部切り欠いた説明図6 to 7 are partially cut explanatory views showing a conventional example.

【図8】従来例の受信波のゼロクロス点に対する妨害波
の干渉例を示す説明用線図
FIG. 8 is an explanatory diagram showing an interference example of an interfering wave with respect to a zero cross point of a received wave in a conventional example.

【図9】従来例の受信波の状態を示す線図FIG. 9 is a diagram showing a state of a received wave in a conventional example.

【符号の説明】[Explanation of symbols]

1 振動子保持部材 2 支持部材 3 弾性部材 4 弾性部材 6 超音波振動子 20 配管 21 フローブホルダ 1 Vibrator Holding Member 2 Support Member 3 Elastic Member 4 Elastic Member 6 Ultrasonic Transducer 20 Piping 21 Flobe Holder

Claims (3)

【実用新案登録請求の範囲】[Scope of utility model registration request] 【請求項1】 超音波振動子を一端部に装備した振動子
保持体と、この振動子保持体を支持する支持部材とを備
えた超音波プローブにおいて、前記振動子保持体と支持
部材との間に、吸振部材を介装したことを特徴とする超
音波プローブ。
1. An ultrasonic probe comprising a vibrator holder having an ultrasonic vibrator at one end, and a support member for supporting the vibrator holder, wherein the vibrator holder and the support member are provided. An ultrasonic probe having a vibration absorbing member interposed therebetween.
【請求項2】 前記吸振部材が、少なくとも前記超音波
振動子の振動方向に沿った方向の吸振機能を備えている
ことを特徴とする請求項1記載の超音波プローブ。
2. The ultrasonic probe according to claim 1, wherein the vibration absorbing member has at least a vibration absorbing function in a direction along a vibration direction of the ultrasonic transducer.
【請求項3】 配管を介して所定距離を隔てて配設され
た流量測定用の一対の超音波プローブと、この超音波プ
ローブを前記配管の軸線に対して所定の傾斜角をもって
着脱自在に且つ密封状態に装備するプローブホルダとを
備え、前記超音波プローブを、振動子保持体とこれを支
持する支持部材とを有し且つ当該振動子保持体と支持部
材との間に吸振部材を備えたものを使用することを特徴
とする超音波流量計。
3. A pair of ultrasonic probes for flow rate measurement, which are arranged at a predetermined distance through a pipe, and the ultrasonic probe is detachable at a predetermined inclination angle with respect to the axis of the pipe. A probe holder mounted in a sealed state, the ultrasonic probe having a vibrator holder and a support member supporting the vibrator holder, and a vibration absorbing member provided between the vibrator holder and the support member. An ultrasonic flow meter characterized by using one.
JP4881991U 1991-05-31 1991-05-31 Ultrasonic probe and ultrasonic flowmeter using the same Expired - Lifetime JPH0716977Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4881991U JPH0716977Y2 (en) 1991-05-31 1991-05-31 Ultrasonic probe and ultrasonic flowmeter using the same

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4881991U JPH0716977Y2 (en) 1991-05-31 1991-05-31 Ultrasonic probe and ultrasonic flowmeter using the same

Publications (2)

Publication Number Publication Date
JPH04134023U JPH04134023U (en) 1992-12-14
JPH0716977Y2 true JPH0716977Y2 (en) 1995-04-19

Family

ID=31927106

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4881991U Expired - Lifetime JPH0716977Y2 (en) 1991-05-31 1991-05-31 Ultrasonic probe and ultrasonic flowmeter using the same

Country Status (1)

Country Link
JP (1) JPH0716977Y2 (en)

Also Published As

Publication number Publication date
JPH04134023U (en) 1992-12-14

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