JPH0532732Y2 - - Google Patents

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Publication number
JPH0532732Y2
JPH0532732Y2 JP1985116490U JP11649085U JPH0532732Y2 JP H0532732 Y2 JPH0532732 Y2 JP H0532732Y2 JP 1985116490 U JP1985116490 U JP 1985116490U JP 11649085 U JP11649085 U JP 11649085U JP H0532732 Y2 JPH0532732 Y2 JP H0532732Y2
Authority
JP
Japan
Prior art keywords
ultrasonic
fluid
flow rate
tube body
flow
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
JP1985116490U
Other languages
Japanese (ja)
Other versions
JPS6225821U (en
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 filed Critical
Priority to JP1985116490U priority Critical patent/JPH0532732Y2/ja
Publication of JPS6225821U publication Critical patent/JPS6225821U/ja
Application granted granted Critical
Publication of JPH0532732Y2 publication Critical patent/JPH0532732Y2/ja
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【考案の詳細な説明】 [産業上の利用分野] 本考案は超音波流速流量計に係り、特に超音波
振動子ユニツト(以下単にユニツトと称する)の
測定用の管体への取付け構造に関する。
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to an ultrasonic flowmeter, and particularly to a structure for attaching an ultrasonic transducer unit (hereinafter simply referred to as a unit) to a measuring tube.

[従来の技術] 流体を超音波の伝搬媒質として、その伝搬時間
により流体の流速や流量を測定する超音波流速流
量計は、従来より広く利用されている。
[Prior Art] Ultrasonic flowmeters that use fluid as a propagation medium for ultrasonic waves and measure the flow rate and flow rate of the fluid based on the propagation time have been widely used.

この種の超音波流速流量計としては特開昭57−
77915号公報によつて開示されたものがある。こ
の提案は第4図に示すように、管体1の対向する
位置における流体の流れ方向を斜めに横切る線上
に、一対の振動子ハウジング2,3がそれぞれ一
体に形成されている。これらの振動子ハウジング
2,3にはそれぞれユニツト4,5がねじなどを
介して装着されている。そして一方のユニツト4
または5から流体中へ超音波信号を放射し他方の
ユニツト5または4で受信し、これらの送受信を
交互に繰りかえして超音波信号の伝搬方向による
伝搬時間の差及び和によつて流体の流速または流
量を計測するように構成されていた。
As this type of ultrasonic flowmeter, the
There is one disclosed in Publication No. 77915. In this proposal, as shown in FIG. 4, a pair of vibrator housings 2 and 3 are integrally formed on a line diagonally crossing the fluid flow direction at opposing positions of the tube body 1. Units 4 and 5 are attached to these vibrator housings 2 and 3, respectively, via screws or the like. And one unit 4
Alternatively, an ultrasonic signal is emitted into the fluid from unit 5 or 4 and received by the other unit 5 or 4, and these transmissions and receptions are repeated alternately to determine the fluid flow velocity or It was configured to measure the flow rate.

[考案が解決しようとする問題点] しかしながら上述した提案のように、対向する
ユニツト4,5が同一線上に配設されていると、
ユニツト4から5の方向に超音波が発射される場
合と、逆方向に発射される場合とでは、流体の流
速と超音波の振幅との関係を示す曲線は第5図に
それぞれ実線と破線で示すように異なる。すなわ
ち、例えば流体が管体1内を矢印A方向に+1.5
/secの流速で流れる場合に、ユニツト4から
5の方向に流体の流れ方向Aと順方向に超音波が
発射されたときの超音波の振幅は、電圧変換され
て約1.6Vとなるが、その逆に超音波が発射され
た場合には約3Vとなる。また流体の流れが矢印
B方向の場合には、同様に超音波が流体の流れ方
向Bと順方向の場合には−1.5/secの流速にお
いて振幅は1.6Vとなり逆方向の場合には3Vとな
る。この場合超音波の振幅を電圧として関知でき
る限界は約1Vであるため、測定可能範囲は第5
図に示すab間の流速範囲となり、測定範囲が狭
くなるという問題があつた。
[Problems to be solved by the invention] However, if the opposing units 4 and 5 are arranged on the same line as in the above proposal,
The curves showing the relationship between the flow velocity of the fluid and the amplitude of the ultrasonic waves are shown in Fig. 5 as solid lines and broken lines, respectively, when the ultrasonic waves are emitted in the direction from units 4 to 5 and when they are emitted in the opposite direction. Different as shown. That is, for example, the fluid moves inside the pipe body 1 in the direction of arrow A by +1.5
When the fluid flows at a flow rate of /sec, the amplitude of the ultrasound when it is emitted in the forward direction of the fluid flow direction A from unit 4 to 5 is approximately 1.6V after voltage conversion. Conversely, when ultrasonic waves are emitted, the voltage is approximately 3V. Similarly, when the fluid flow is in the direction of arrow B, the amplitude is 1.6V at a flow rate of -1.5/sec when the ultrasonic wave is in the forward direction of the fluid flow direction B, and 3V when it is in the opposite direction. Become. In this case, the limit to which the amplitude of the ultrasonic wave can be measured as a voltage is approximately 1V, so the measurable range is the fifth
There was a problem that the flow velocity range was between a and b as shown in the figure, and the measurement range became narrow.

本考案の目的は、上記問題を解消し、測定範囲
を広くすることができる超音波流速流量計を提供
することにある。
An object of the present invention is to provide an ultrasonic flowmeter that can solve the above problems and widen the measurement range.

[問題点を解決するための手段] 本考案に係る超音波流速流量計は、流体が流通
する管体に、この流体の流れ方向に傾斜して相対
向するように取付けられ、超音波信号を送受して
前記管体内を通流する流体の流速または流量を測
定する一対の超音波振動子ユニツトからそれぞれ
発射された超音波の中心線が、前記管体の中心線
上で相互に離間した位置において交差する平行線
となるように構成したものである。
[Means for Solving the Problems] The ultrasonic flow meter according to the present invention is installed in a pipe through which a fluid flows so as to be inclined and face each other in the flow direction of the fluid, and transmits an ultrasonic signal. The center lines of the ultrasonic waves respectively emitted from a pair of ultrasonic transducer units that transmit and receive to measure the flow velocity or flow rate of the fluid flowing through the tube body are at positions spaced apart from each other on the center line of the tube body. The lines are arranged in such a way that they are parallel lines that intersect.

[作用] 上記の構成によると、超音波の伝播する方向が
管体内を通流する流体の流れ方向に対し順方向ま
たは逆方向のいずれの場合でも、流体の流速と超
音波の振幅との関係がほぼ同じになり、流体の流
れ方向が変つても流速と超音波の振幅との関係が
ほとんど変らないため、測定範囲を広くすること
ができる。
[Operation] According to the above configuration, the relationship between the flow velocity of the fluid and the amplitude of the ultrasonic wave is maintained regardless of whether the direction in which the ultrasonic wave propagates is in the forward direction or in the opposite direction to the flow direction of the fluid flowing through the tube. are almost the same, and even if the flow direction of the fluid changes, the relationship between the flow velocity and the amplitude of the ultrasonic wave hardly changes, so the measurement range can be widened.

[実施例] 以下、図示の実施例に基づいて本考案を詳細に
説明する。
[Example] Hereinafter, the present invention will be described in detail based on the illustrated example.

第1図は本考案に係る超音波流速流量計の一実
施例を示す断面図である。該図において、第4図
に示す従来例と同一または同等部分には同一符号
を付して示し、説明を省略する。ユニツト4の中
心線4aと管体1の中心線1aとの交点をmと
し、ユニツト5の中心線5aと管体1の中心線1
aとの交点をnとしたばあい、これらの交点m,
nはそれぞれ管体1のB方向、A方向に近い位置
にあり、これらの交点m,n間の距離は約2mmで
ある。そしてこれらの中心線4a,5aは平行で
あり管体1の中心線1aとは約30度の角度をもつ
て交差している。
FIG. 1 is a sectional view showing an embodiment of an ultrasonic flow meter according to the present invention. In this figure, the same or equivalent parts as in the conventional example shown in FIG. 4 are denoted by the same reference numerals, and the explanation thereof will be omitted. The intersection point between the center line 4a of the unit 4 and the center line 1a of the tube body 1 is defined as m, and the center line 5a of the unit 5 and the center line 1 of the tube body 1 are defined as m.
If the intersection with a is n, then these intersections m,
n are located close to the B direction and A direction of the tube body 1, respectively, and the distance between these intersection points m and n is about 2 mm. These center lines 4a and 5a are parallel and intersect with the center line 1a of the tubular body 1 at an angle of about 30 degrees.

上述したように構成された本実施例の作用を以
下に説明する。実験値によれば第2図に示すよう
に前記交点m,n間の距離が0mm,1mm,2mmの
場合には流量と超音波の振幅を電圧に変換した値
との関係はそれぞれ曲線D,E,Fとして示すよ
うになる。ただし実線で示す曲線は管体1内を流
れる流体の流れ方向と順方向に超音波が発射され
た場合であり、破線で示す曲線は超音波が逆方向
に発射された場合である。第2図で示すように交
点m,n間の交点が2mmの場合には超音波の発射
方向がいずれの場合でもほぼ同じ曲線となる。従
つて第3図に示すように管体1内の流体の流速が
例えば±1.5/secの場合に超音波の振幅は電圧
変換した値でいずれも約3Vとなる。この結果関
知できる電圧が1Vとした場合の測定範囲は第5
図に示す従来の測定範囲よりはるかに広くなる。
上述した実施例ではユニツトの取付角度が管体1
の中心線1aに対して約30度であり、ユニツト
4,5の中心線4a,5aと管体1の中心線1a
とのそれぞれの交点m,n間の距離が2mmのとき
に測定範囲が最も広くなる場合について説明した
が、このm,n間の距離は流量計の寸法形状によ
つて変るものであり、この数字に限定されるもの
ではない。
The operation of this embodiment configured as described above will be explained below. According to the experimental values, as shown in Fig. 2, when the distance between the intersections m and n is 0 mm, 1 mm, and 2 mm, the relationship between the flow rate and the value obtained by converting the amplitude of the ultrasonic wave into voltage is curve D, respectively. They will be shown as E and F. However, the curve shown by a solid line is the case where the ultrasonic wave is emitted in the forward direction of the flow direction of the fluid flowing inside the tube body 1, and the curve shown by the broken line is the case where the ultrasonic wave is emitted in the opposite direction. As shown in FIG. 2, if the intersection between the intersections m and n is 2 mm, the curve will be almost the same regardless of the direction in which the ultrasonic waves are emitted. Therefore, as shown in FIG. 3, when the flow rate of the fluid in the tube body 1 is, for example, ±1.5/sec, the amplitude of the ultrasonic wave is approximately 3 V in terms of voltage conversion. As a result, if the voltage that can be detected is 1V, the measurement range is 5th.
This is much wider than the conventional measurement range shown in the figure.
In the embodiment described above, the installation angle of the unit is
It is approximately 30 degrees with respect to the center line 1a of the unit 4, 5, and the center line 1a of the tube body 1.
We have explained the case where the measurement range is widest when the distance between the respective intersections m and n with the It is not limited to numbers.

また管体1内に通流する流体の流速または流量
を測定すると同時に流体中の特定の成分の濃度を
測定するための赤外線検知器をユニツト間に取付
ける場合には、ユニツト間が広くなるので取付け
易いという効果もある。
In addition, if an infrared detector is installed between the units to measure the flow rate or flow rate of the fluid flowing through the pipe body 1 and at the same time the concentration of a specific component in the fluid, the distance between the units will be wide. It also has the effect of being easy.

[考案の効果] 上述したとおり、本考案によれば、超音波流速
流量計の管体に傾斜して儲けた一対のユニツトの
中心線を適当な間隔を有する平行線としたので、
ユニツトから発射される超音波の方向に関係なく
測定範囲を広くすることができる。
[Effects of the invention] As described above, according to the invention, the center lines of the pair of inclined units on the tube body of the ultrasonic flowmeter are made into parallel lines with an appropriate interval.
The measurement range can be widened regardless of the direction of the ultrasonic waves emitted from the unit.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本考案に係る超音波流速流量計の一実
施例を示す断面図、第2図、第3図は流速と超音
波の振幅の関係を示すグラフ、第4図は従来の超
音波流速流量計を示す断面図、第5図は第4図に
示す流量計の流速と超音波の振幅の関係を示すグ
ラフである。 1……管体、1a……管体の中心線、4,5…
…超音波振動子ユニツト、4a,5a……超音波
振動子の中心線。
Fig. 1 is a sectional view showing an embodiment of an ultrasonic flowmeter according to the present invention, Figs. 2 and 3 are graphs showing the relationship between flow velocity and ultrasonic amplitude, and Fig. 4 is a graph showing a conventional ultrasonic flowmeter. FIG. 5 is a cross-sectional view showing the flow rate meter, and is a graph showing the relationship between the flow rate of the flow meter shown in FIG. 4 and the amplitude of ultrasonic waves. 1... tube body, 1a... center line of tube body, 4, 5...
...Ultrasonic transducer unit, 4a, 5a... Center line of ultrasonic transducer.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 流体が通流する管体に、この流体の流れ方向に
傾斜して相対向するように取付けられ、超音波信
号を送受して前記管体内を通流する流体の流速ま
たは流量を測定する一対の超音波振動子ユニツト
を具備した超音波流速流量計において、前記一対
の超音波振動子からそれぞれ発射された超音波の
中心線が前記管体の中心線上で相互に離間した位
置において交差する平行線であることを特徴とす
る超音波流速流量計。
A pair of tubes that are attached to a tube through which a fluid flows so as to face each other while being inclined in the flow direction of the fluid, and transmit and receive ultrasonic signals to measure the flow rate or flow rate of the fluid flowing through the tube. In an ultrasonic flowmeter equipped with an ultrasonic transducer unit, parallel lines where the center lines of the ultrasonic waves respectively emitted from the pair of ultrasonic transducers intersect at positions spaced apart from each other on the center line of the tube body. An ultrasonic flow rate meter characterized by:
JP1985116490U 1985-07-31 1985-07-31 Expired - Lifetime JPH0532732Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1985116490U JPH0532732Y2 (en) 1985-07-31 1985-07-31

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1985116490U JPH0532732Y2 (en) 1985-07-31 1985-07-31

Publications (2)

Publication Number Publication Date
JPS6225821U JPS6225821U (en) 1987-02-17
JPH0532732Y2 true JPH0532732Y2 (en) 1993-08-20

Family

ID=31001129

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1985116490U Expired - Lifetime JPH0532732Y2 (en) 1985-07-31 1985-07-31

Country Status (1)

Country Link
JP (1) JPH0532732Y2 (en)

Also Published As

Publication number Publication date
JPS6225821U (en) 1987-02-17

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