JP3259201B2 - Flowmeter - Google Patents
FlowmeterInfo
- Publication number
- JP3259201B2 JP3259201B2 JP14022093A JP14022093A JP3259201B2 JP 3259201 B2 JP3259201 B2 JP 3259201B2 JP 14022093 A JP14022093 A JP 14022093A JP 14022093 A JP14022093 A JP 14022093A JP 3259201 B2 JP3259201 B2 JP 3259201B2
- Authority
- JP
- Japan
- Prior art keywords
- ultrasonic
- receivers
- frequency band
- transmitter
- pipe
- 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
Links
Landscapes
- Measuring Volume Flow (AREA)
Description
【0001】[0001]
【産業上の利用分野】本発明は、超音波を用いた流量計
に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a flow meter using ultrasonic waves.
【0002】[0002]
【従来の技術】従来、超音波を用いた流量計の一例とし
てガスを被測定流体とするガス用超音波渦流量計があ
る。このガス用超音波渦流量計は、被測定流体であるガ
スを通す管路と、この管路中に設けて下流側にカルマン
渦を発生させる渦発生体と、ガス中に超音波を放射する
超音波送信器と、この超音波送信器からの超音波をガス
中のカルマン渦を通して受信する超音波受信器と、この
超音波受信器からの信号に基づいて流量に比例した流量
信号を出力する演算回路とから大略構成されておりカル
マン渦による超音波の周波数変調度合いが流量に比例す
ることを利用したものになっている。そして、このガス
用超音波渦流量計は、ガス中に超音波を放射し、カルマ
ン渦から受けた周波数変調を演算回路で復調してカルマ
ン渦の発生数を検出しこのカルマン渦の発生数に基づい
てガスの流速、ひいては流量を計測している。2. Description of the Related Art Conventionally, as an example of a flow meter using ultrasonic waves, there is an ultrasonic vortex flow meter for gas using gas as a fluid to be measured. This gas ultrasonic vortex flowmeter radiates ultrasonic waves into the gas, and a vortex generator that is provided in the pipe and generates a Karman vortex on the downstream side. An ultrasonic transmitter, an ultrasonic receiver that receives ultrasonic waves from the ultrasonic transmitter through Karman vortices in gas, and outputs a flow signal proportional to a flow rate based on a signal from the ultrasonic receiver. It is generally composed of an arithmetic circuit and utilizes the fact that the degree of frequency modulation of ultrasonic waves by Karman vortices is proportional to the flow rate. The ultrasonic vortex flowmeter for gas emits ultrasonic waves into the gas, demodulates the frequency modulation received from the Karman vortex with an arithmetic circuit, detects the number of generated Karman vortices, and calculates the number of generated Karman vortices. The flow velocity of the gas, and hence the flow rate, is measured based on the measured flow velocity.
【0003】[0003]
【発明が解決しようとする課題】ところで、ガス中は超
音波が比較的伝播しにくいため、受信電圧が低く、受信
可能周波数帯域も狭くなってしまう。そして、高流量に
なるほど周波数変調度合いは大きくなるため、高流量時
の伝播超音波周波数が受信可能周波数帯域を超えてしま
い受信できなくなる虞があった。また、受信可能周波数
帯域が狭いことから超音波送信器と超音波受信器の共振
周波数を精度高く整合しなければならず、特性管理が容
易でなかった。上述した問題点の改善のために受信可能
周波数帯域が広い超音波受信器を用いることが考えられ
るが、素子の特性や構造上の制約があること等によりそ
のままの適用を図れないというのが実情であった。By the way, since ultrasonic waves are relatively hard to propagate in gas, the receiving voltage is low and the receivable frequency band is narrow. Since the degree of frequency modulation increases as the flow rate increases, the transmitted ultrasonic frequency at the time of the high flow rate exceeds the receivable frequency band, and there is a possibility that reception becomes impossible. In addition, since the receivable frequency band is narrow, the resonance frequencies of the ultrasonic transmitter and the ultrasonic receiver must be matched with high accuracy, and the characteristic management is not easy. It is conceivable to use an ultrasonic receiver with a wide receivable frequency band in order to improve the above-mentioned problems. However, in reality, it cannot be applied as it is due to restrictions on the characteristics and structure of elements. Met.
【0004】本発明は、上記事情に鑑みてなされたもの
で、広い周波数範囲で安定して超音波を受信できる流量
計を提供することを目的とする。[0004] The present invention has been made in view of the above circumstances, and has as its object to provide a flowmeter capable of receiving ultrasonic waves stably in a wide frequency range.
【0005】[0005]
【課題を解決するための手段】本発明は、上記目的を達
成するために、流体が流通する管路と、該管路中に設け
て下流側にカルマン渦を発生させる渦発生体と、該管路
中の流体に対して超音波を放射する超音波送信器と、該
超音波送信器からの超音波をカルマン渦を通して受信す
る複数個の超音波受信器と、複数個の超音波受信器から
の信号に基づいて流量に比例した流量信号を出力する演
算回路とを備え、前記複数個の超音波受信器は、それぞ
れの受信可能周波数帯域を相互にずらしてかつ一部を重
畳させて設定したことを特徴とする。In order to achieve the above object, the present invention provides a pipe through which a fluid flows, and a pipe provided in the pipe.
A vortex generator for generating Karman vortices downstream Te, an ultrasonic transmitter that radiates ultrasonic waves to the fluid in the conduit, receives the ultrasonic wave from the ultrasonic transmitter through the Karman vortex A plurality of ultrasonic receivers, and an arithmetic circuit that outputs a flow signal proportional to the flow rate based on signals from the plurality of ultrasonic receivers, wherein the plurality of ultrasonic receivers The present invention is characterized in that receivable frequency bands are set to be shifted from each other and partially overlapped.
【0006】[0006]
【作用】このような構成とすれば、全体の受信可能周波
数帯域を超音波送信器の送信可能周波数帯域より広い範
囲に設定でき、このように設定することにより超音波送
信器から超音波が放射されてカルマン渦により変調を受
けても、変調された超音波を広範囲の周波数に亙って受
信することになる。複数個の超音波受信器の受信可能周
波数帯域を少しずらして設定することにより広範囲にわ
たって超音波を受信できるので、超音波送信器、複数個
の超音波受信器の共振周波数の精度高い整合を行わなく
て済む。このため、共振周波数の精度高い整合を省略す
る分特性管理を緩和でき、ひいては製作の簡素化を図る
ことができる。With this configuration, the entire receivable frequency band can be set to a range wider than the transmittable frequency band of the ultrasonic transmitter, and the ultrasonic transmitter emits ultrasonic waves by setting in this manner. Even if it is modulated by the Karman vortex, the modulated ultrasonic waves will be received over a wide range of frequencies. By setting the receivable frequency bands of a plurality of ultrasonic receivers to be slightly shifted, ultrasonic waves can be received over a wide range, so that the ultrasonic transmitters and the plurality of ultrasonic receivers are accurately matched in resonance frequency. You don't have to. For this reason, the characteristic management can be eased by omitting the high-precision matching of the resonance frequency, and the production can be simplified.
【0007】[0007]
【実施例】以下、本発明の一実施例の流量計を図1及び
図2に基づいて説明する。図において、ガス等の流体を
通す管路1には、下流側にカルマン渦を発生させる渦発
生体2が設けられている。管路1のカルマン渦発生領域
には、流体の流れの情報を得るための超音波送信器3、
第1、第2の超音波受信器4,5が同一円周上に並んで
設けられている。そして、超音波送信器3に接続した発
振器6が発生した超音波信号Jを超音波送信器3が流体
中に放射すると、流体中を伝播する超音波がカルマン渦
により流量に対応した変調を受けて第1、第2の超音波
受信器4,5に受信されるようになっている。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS A flow meter according to an embodiment of the present invention will be described below with reference to FIGS. In the drawing, a vortex generator 2 for generating Karman vortices is provided on a downstream side of a pipe 1 through which a fluid such as gas flows. In the Karman vortex generation region of the pipe 1, an ultrasonic transmitter 3 for obtaining information on the flow of the fluid,
First and second ultrasonic receivers 4 and 5 are provided side by side on the same circumference. When the ultrasonic transmitter 3 radiates the ultrasonic signal J generated by the oscillator 6 connected to the ultrasonic transmitter 3 into the fluid, the ultrasonic waves propagating in the fluid are modulated by the Karman vortex according to the flow rate. The first and second ultrasonic receivers 4 and 5 receive the signals.
【0008】超音波送信器3は、図2(a)に示すよう
に周波数f0 を中心にした送信可能周波数帯域Aを設定
したものになっている。第1の超音波受信器4には、図
2(b)に示すように周波数f0 を最小値とする受信可
能周波数帯域Bを設定し、第2の超音波受信器5には、
図2(b)に示すように周波数f1 (f0 <f1 )を最
大値とする受信可能周波数帯域Cを設定しており、この
第1、第2の超音波受信器4,5は、それぞれの受信可
能周波数帯域B,Cがずれ、かつ周波数f0 ないしf1
の部分で重畳して全体の受信可能周波数帯域Dが連続し
たものになっている。As shown in FIG. 2A, the ultrasonic transmitter 3 sets a transmittable frequency band A centered on a frequency f 0 . As shown in FIG. 2B, a receivable frequency band B that minimizes the frequency f 0 is set for the first ultrasonic receiver 4, and the second ultrasonic receiver 5 is set for the second ultrasonic receiver 5.
As shown in FIG. 2B, a receivable frequency band C having a maximum value of the frequency f 1 (f 0 <f 1 ) is set, and the first and second ultrasonic receivers 4, 5 , The respective receivable frequency bands B and C are shifted, and the frequencies f 0 to f 1
Are superimposed at the portion, and the entire receivable frequency band D is continuous.
【0009】第1、第2の超音波受信器4,5及び発振
器6に接続して演算回路7が設けられている。演算回路
7は、第1、第2の超音波受信器4,5に接続した第
1、第2の増幅器8,9と、第1、第2の増幅器8,9
から信号を入力してこの信号を復調する復調器10と、復
調器10からの信号に基づいて流量に比例した流量信号K
を出力する出力回路11とから構成されている。An arithmetic circuit 7 is connected to the first and second ultrasonic receivers 4 and 5 and the oscillator 6. The arithmetic circuit 7 includes first and second amplifiers 8 and 9 connected to the first and second ultrasonic receivers 4 and 5, and first and second amplifiers 8 and 9,
And a demodulator 10 for inputting a signal from the demodulator and demodulating the signal, and a flow signal K proportional to the flow rate based on the signal from the demodulator 10.
And an output circuit 11 for outputting the same.
【0010】このように構成された流量計では、全体の
受信可能周波数帯域Dが超音波送信器3の送信可能周波
数帯域Aより広い範囲に設定されることになり、超音波
送信器3から超音波が放射されてカルマン渦により変調
を受けても、変調された超音波を確実に受信して流量を
精度高く計測できる。さらに、仮に流体の流れが高流量
になって周波数変調度合いが大きくなってもこれを受信
して流量を適正に計測できることになる。In the flowmeter configured as described above, the entire receivable frequency band D is set to a range wider than the receivable frequency band A of the ultrasonic transmitter 3, and the ultrasonic transmitter 3 Even if a sound wave is emitted and is modulated by the Karman vortex, the modulated ultrasonic wave can be reliably received and the flow rate can be measured with high accuracy. Further, even if the flow of the fluid becomes a high flow rate and the degree of frequency modulation becomes large, it can be received and the flow rate can be properly measured.
【0011】上述したように第1、第2の超音波受信器
4,5のそれぞれの受信可能周波数帯域B,Cを少しず
らして設定することにより広範囲にわたって超音波を受
信できるので、超音波送信器3、第1、第2の超音波受
信器4,5の共振周波数を精度高く整合しなくて済む。
このため、共振周波数の精度高い整合を省略する分特性
管理を緩和でき、ひいては製作の簡素化を図ることがで
きる。As described above, by setting the receivable frequency bands B and C of the first and second ultrasonic receivers 4 and 5 to be slightly shifted, ultrasonic waves can be received over a wide range. It is not necessary to match the resonance frequencies of the receiver 3, the first and second ultrasonic receivers 4, 5 with high accuracy.
For this reason, the characteristic management can be eased by omitting the high-precision matching of the resonance frequency, and the production can be simplified.
【0012】本実施例では、超音波受信器が第1、第2
の超音波受信器4,5の二つである場合を例にしたが、
三つ以上の超音波受信器を用いるようにしてもよい。ま
た、本実施例では、超音波送信器3、第1、第2の超音
波受信器4,5が同一円周上に並んで設けられている場
合を例にしたが、これに限定されるものでなく、送受信
可能の位置であれば任意の位置に設けるようにしてもよ
い。In this embodiment, the ultrasonic receivers are first and second ultrasonic receivers.
As an example, two ultrasonic receivers 4 and 5 were used.
Three or more ultrasonic receivers may be used. Further, in the present embodiment, the case where the ultrasonic transmitter 3, the first and second ultrasonic receivers 4, 5 are provided side by side on the same circumference is taken as an example, but the present invention is not limited to this. Instead, it may be provided at any position as long as it can transmit and receive.
【0013】[0013]
【発明の効果】本発明は、以上説明したように構成され
た流量計であるから、全体の受信可能周波数帯域を超音
波送信器の送信可能周波数帯域より広い範囲に設定して
カルマン渦により変調された超音波を広範囲の周波数に
亙って受信するので、流量を精度高くかつ安定して計測
できる。複数個の超音波受信器の受信可能周波数帯域を
少しずらして設定することにより広範囲にわたって超音
波を受信して超音波送信器、複数個の超音波受信器の共
振周波数の精度高い整合を行わなくて済むので、共振周
波数の精度高い整合を省略する分、特性管理を緩和で
き、ひいては製作の簡素化を図ることができる。Since the present invention is a flow meter constructed as described above, the whole receivable frequency band is set to a range wider than the transmittable frequency band of the ultrasonic transmitter and modulated by Karman vortex. Since the transmitted ultrasonic waves are received over a wide range of frequencies, the flow rate can be measured accurately and stably. By setting the receivable frequency bands of a plurality of ultrasonic receivers to be slightly shifted, ultrasonic waves are received over a wide range and the ultrasonic transmitter does not perform high-precision matching of the resonance frequencies of the plural ultrasonic receivers. Since the matching of the resonance frequency with high accuracy is omitted, the characteristic management can be eased, and the production can be simplified.
【図1】本発明の一実施例の流量計を模式的に示す図で
ある。FIG. 1 is a diagram schematically showing a flow meter according to one embodiment of the present invention.
【図2】同流量計の超音波送信器、第1、第2の超音波
受信器の周波数帯域を示す特性図である。FIG. 2 is a characteristic diagram showing frequency bands of an ultrasonic transmitter and first and second ultrasonic receivers of the flow meter.
1 管路 3 超音波送信器 4 第1の超音波受信器 5 第2の超音波受信器 7 演算回路 B 第1の超音波受信器の受信可能周波数帯域 C 第2の超音波受信器の受信可能周波数帯域 D 全体の受信可能周波数帯域 Reference Signs List 1 conduit 3 ultrasonic transmitter 4 first ultrasonic receiver 5 second ultrasonic receiver 7 arithmetic circuit B receivable frequency band of first ultrasonic receiver C reception of second ultrasonic receiver Possible frequency band D Overall receivable frequency band
───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 平6−288800(JP,A) 特開 昭64−78114(JP,A) 特開 平3−274418(JP,A) (58)調査した分野(Int.Cl.7,DB名) G01F 1/32 ──────────────────────────────────────────────────続 き Continuation of the front page (56) References JP-A-6-288800 (JP, A) JP-A-64-78114 (JP, A) JP-A-3-274418 (JP, A) (58) Field (Int.Cl. 7 , DB name) G01F 1/32
Claims (1)
て下流側にカルマン渦を発生させる渦発生体と、該管路
中の流体に対して超音波を放射する超音波送信器と、該
超音波送信器からの超音波をカルマン渦を通して受信す
る複数個の超音波受信器と、複数個の超音波受信器から
の信号に基づいて流量に比例した流量信号を出力する演
算回路とを備え、前記複数個の超音波受信器は、それぞ
れの受信可能周波数帯域を相互にずらしてかつ一部を重
畳させて設定したことを特徴とする流量計。1. A pipe through which a fluid flows, and a pipe provided in the pipe.
A vortex generator for generating Karman vortices downstream Te, an ultrasonic transmitter that radiates ultrasonic waves to the fluid in the conduit, receives the ultrasonic wave from the ultrasonic transmitter through the Karman vortex A plurality of ultrasonic receivers, and an arithmetic circuit that outputs a flow signal proportional to the flow rate based on signals from the plurality of ultrasonic receivers, wherein the plurality of ultrasonic receivers A flowmeter wherein receivable frequency bands are set to be shifted from each other and partially overlapped.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP14022093A JP3259201B2 (en) | 1993-05-19 | 1993-05-19 | Flowmeter |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP14022093A JP3259201B2 (en) | 1993-05-19 | 1993-05-19 | Flowmeter |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH06331403A JPH06331403A (en) | 1994-12-02 |
| JP3259201B2 true JP3259201B2 (en) | 2002-02-25 |
Family
ID=15263706
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP14022093A Expired - Fee Related JP3259201B2 (en) | 1993-05-19 | 1993-05-19 | Flowmeter |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP3259201B2 (en) |
-
1993
- 1993-05-19 JP JP14022093A patent/JP3259201B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPH06331403A (en) | 1994-12-02 |
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