JPH0648351Y2 - Vortex flowmeter signal amplification circuit - Google Patents

Vortex flowmeter signal amplification circuit

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Publication number
JPH0648351Y2
JPH0648351Y2 JP1988148227U JP14822788U JPH0648351Y2 JP H0648351 Y2 JPH0648351 Y2 JP H0648351Y2 JP 1988148227 U JP1988148227 U JP 1988148227U JP 14822788 U JP14822788 U JP 14822788U JP H0648351 Y2 JPH0648351 Y2 JP H0648351Y2
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JP
Japan
Prior art keywords
vortex
amplification circuit
flexible
signal amplification
flexible cylinder
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
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JP1988148227U
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Japanese (ja)
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JPH0269719U (en
Inventor
勝夫 三角
秀一 佐藤
Original Assignee
オーバル機器工業株式会社
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Priority to JP1988148227U priority Critical patent/JPH0648351Y2/en
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Description

【考案の詳細な説明】 技術分野 本考案は、渦流量計の信号増幅回路,より詳細には、渦
発生体と別体に構成された片持式の渦検出器の振動雑音
を渦信号から除去して増幅する信号増幅回路に関する。
TECHNICAL FIELD The present invention relates to a signal amplification circuit of a vortex flowmeter, and more specifically, to the vibration noise of a cantilever type vortex detector separately formed from a vortex generator from the vortex signal. The present invention relates to a signal amplification circuit that removes and amplifies.

従来技術 渦流量計の渦検出方式として、従来、渦発生に伴って生
ずる変動圧による歪信号として検知するものが多く採用
されているが、これは、この方式の渦検出手段が、被側
流体に接することがなく、信頼性が高いという特徴をも
っているためである。この方式には、渦発生体を起歪体
とし、該起歪体に生ずる歪または応力の変化として渦を
検出する検出素子を渦発生体の内又は外に埋設して一体
化する方式のものと、渦発生体と別体的に構成された渦
検出器を穿孔された圧力検知室に内壁と非接触に挿入
し、一端を渦発生体端部または流管壁に固設し渦発生体
の両側面に開口し圧力検知室に導通する圧力導通孔を介
して作用する渦変動圧力を検出する方式ものもと、渦発
生体の後流側に一端を固設して渦変動圧力を検出する方
式のものとがある。渦検出器を渦発生体と別体的にした
後述の2方式のものは広い範囲の口径の流量計に対し
て、同一の渦検出器を適用すること、並びに、小形で可
撓性のある検出器とすることができるので、高感度に渦
を検出し易いという長所がある。特に、渦検出器を別体
的に構成し、渦発生体内に挿入した前述の第2の方式は
渦発生体を一体的に構成することができるので、渦検出
素子を埋設した第1の方式と同様に簡易小形な渦流量計
を構成することができる。第2の方式には、先に本出願
人の提案した特公昭63−31726号公報に開示されたもの
がある。該公報の渦検出器は可撓筒内に短冊状母材に歪
検出素子を固着した歪検出要素を挿入した歪検出方式で
ある。更に、特開昭62−215829号公報に提案された渦検
出器は、渦変動圧力に応動する可撓筒と、該可撓筒内に
緩挿された電極支持部材とからなり、渦信号を該電極支
持部材に設けられた少なくとも一個の固定電極と可撓筒
を変動電極とした静電容量の変化として検出する静歪容
量検出方式である。このような渦検出器を渦発生体と別
体的に設ける方式は、高感度に渦変動圧力を検出できる
ので小流量域での流量計測を可能として流量計測範囲を
拡大することができる。渦変動圧力は流速の2乗に比例
するので、渦検出器が圧力に比例した出力が得られると
すると、渦信号は計測範囲の2乗に比例して+40dB/Dec
の傾斜をもって増大する。一方、この渦信号を信号処理
するプリアンプは、流速の測定範囲において信号レベル
が一定となるゲイン特性のものが望ましいが、低域にお
ける配管振動ノイズ、高域における流体振動ノイズ等を
除くため、第7図に示すごとく、低域においては所定の
渦周波数に遮断周波数faに向けて+20dB/Decで増加する
増幅特性のプリアンプと、高域においては所定の渦周波
数に遮断周波数fbをもち−40〜−80dB/Decで減衰するア
クティブフィルタ等を組合せて好適な周波数特性を与え
ている。
2. Description of the Related Art Conventionally, as a vortex detecting method of a vortex flowmeter, a method of detecting as a strain signal due to a fluctuating pressure generated due to the generation of a vortex has been widely adopted. This is because it has high reliability because it does not come into contact with. In this method, a vortex generator is used as a flexure element, and a detection element that detects a vortex as a change in strain or stress generated in the flexure element is embedded inside or outside the vortex generator to be integrated. The vortex generator, which is configured separately from the vortex generator, is inserted into the perforated pressure detection chamber without contact with the inner wall, and one end is fixed to the vortex generator end or the flow tube wall. The vortex fluctuating pressure acting through the pressure communicating hole that opens to both sides of the vortex generator and communicates with the pressure detection chamber is detected.The vortex fluctuating pressure is detected by fixing one end to the wake side of the vortex generator. There is a method to do. The vortex detector separate from the vortex generator, which will be described later, applies the same vortex detector to a wide range of flowmeters, and is small and flexible. Since it can be used as a detector, it has an advantage that it is easy to detect a vortex with high sensitivity. In particular, the above-mentioned second method in which the vortex detector is separately configured and inserted in the vortex generator can be configured integrally with the vortex generator, so that the first method in which the vortex detecting element is embedded is used. Similarly, a simple and small vortex flowmeter can be constructed. The second method is disclosed in Japanese Patent Publication No. Sho 63-31726 previously proposed by the present applicant. The vortex detector of the publication is a strain detection system in which a strain detection element having a strain detection element fixed to a strip-shaped base material is inserted in a flexible cylinder. Further, the vortex detector proposed in Japanese Patent Laid-Open No. 62-215829 is composed of a flexible cylinder that responds to vortex fluctuation pressure, and an electrode support member that is loosely inserted in the flexible cylinder, and outputs a vortex signal. This is a static strain capacitance detection method in which at least one fixed electrode and a flexible cylinder provided on the electrode support member are used as variable electrodes to detect a change in capacitance. In the method in which such a vortex detector is provided separately from the vortex generator, the vortex fluctuation pressure can be detected with high sensitivity, so that the flow rate can be measured in a small flow rate range and the flow rate measurement range can be expanded. Since the vortex fluctuation pressure is proportional to the square of the flow velocity, if the vortex detector can obtain an output proportional to the pressure, the vortex signal will be +40 dB / Dec in proportion to the square of the measurement range.
Increases with the slope of. On the other hand, it is desirable that the preamplifier that processes this vortex signal has a gain characteristic that the signal level is constant in the measurement range of the flow velocity, but in order to exclude pipe vibration noise in the low range, fluid vibration noise in the high range, etc. As shown in Fig. 7, it has a preamplifier with an amplification characteristic that increases by +20 dB / Dec toward the cutoff frequency fa at a predetermined vortex frequency in the low frequency range, and has a cutoff frequency fb at the predetermined vortex frequency in the high frequency range from -40 to A suitable frequency characteristic is given by combining an active filter that attenuates at -80 dB / Dec.

従来技術の問題点 上述のごとく、渦発生体と別体に設けられた渦検出器と
をもった渦流量計は、高感度に微小圧力に応動し、小流
感度は向上するが、渦検出器の固有振動数f0が雑音とな
りS/Nを悪化させるため、該固有振動数f0に渦信号の周
波数が近接する高流域の上限値が制限される。高流域を
伸ばすためには渦検出器の固有振動数を高くすることで
あるが、このことは剛性を高めることにより、逆に少流
量の計測限界を低下させ、最大渦信号周波数fはf=0.
2f0が限界であった。
Problems of the Prior Art As described above, the vortex flowmeter having the vortex generator and the vortex detector separately provided responds to minute pressure with high sensitivity and improves small flow sensitivity, but vortex detection since the natural frequency f 0 of the vessel exacerbates the S / N becomes noise, the upper limit of the high basin adjacent the frequency of the vortex signal to said intrinsic vibration frequency f 0 is limited. In order to extend the high flow region, the natural frequency of the vortex detector is increased, but this increases rigidity, which lowers the measurement limit for small flow rates, and the maximum vortex signal frequency f is f = 0.
The limit was 2f 0 .

第8図及び第9図は、所定流量における周波数fと固有
振動数f0の周波数成分の関係((a)図)と、渦信号波
形((b図))の例を示したもので、第8図は、f=0.
182f0の場合であるが、固有振動数f0=3200Hzの雑音成
分が、すでに渦信号を乱していることを示している。ま
た、第9図は、f=0.344f0の場合であるが、この場
合、渦信号を性格に判別することは困難となっている。
8 and 9 show an example of the relationship between the frequency f and the frequency component of the natural frequency f 0 at a predetermined flow rate ((a)) and the vortex signal waveform ((b)). In FIG. 8, f = 0.
In the case of 182f 0 , it is shown that the noise component of natural frequency f 0 = 3200Hz has already disturbed the vortex signal. Further, FIG. 9 shows the case of f = 0.344f 0 , but in this case, it is difficult to distinguish the eddy signal from the character.

上述の如く、高流域においては渦検出器の固有振動が主
な雑音源になっており、この雑音を除去するには更に高
次の減衰をもつフィルタを追加しなければならず、この
結果回路が複雑となり高価になるという欠点があった。
As mentioned above, the natural vibration of the vortex detector is the main noise source in the high flow region, and in order to remove this noise, it is necessary to add a filter with higher-order attenuation. Has the drawback of being complicated and expensive.

問題点解決のための手段 本考案は、上述した従来技術の問題点に鑑みなされたも
ので、渦検出器の固有振動数成分を除去してS/Nを改善
し、小流量の感度を損うことなく、大流量域の流量計測
を拡大可能として流量範囲の優れた渦流量計を安価に提
供することを目的とする。即ち、流管と、該流管内に流
れに対向して配設された渦発生体と、一端は、前期流管
又は渦発生体に固定し、他端は渦の変動圧力に応動して
変位する可撓体で、該可撓大の変位を検出する片持式の
渦検出器と該渦検出器で検知された渦信号に含まれた雑
音成分を除去するフィルタ回路を有する渦変換器とから
なり、流量に応じて変化する渦信号から流量を求める渦
流量計において、前期フィルタ回路に片持式渦検出器の
固有振動数をnu11周波数とするノッチフィルタを具備し
た渦流量計信号増幅回路を提供するものである。
Means for Solving Problems The present invention has been made in view of the above-mentioned problems of the conventional technology, and removes the natural frequency component of the vortex detector to improve the S / N and impair the sensitivity of a small flow rate. It is an object of the present invention to provide a vortex flowmeter with an excellent flow rate range at low cost by expanding the flow rate measurement in a large flow rate range without any need. That is, the flow tube and the vortex generator disposed in the flow tube so as to face the flow are fixed at one end to the former flow tube or vortex generator, and the other end is displaced in response to the fluctuating pressure of the vortex. A cantilever type vortex detector for detecting the large displacement of the flexible body, and a vortex converter having a filter circuit for removing a noise component contained in the vortex signal detected by the vortex detector. In a vortex flowmeter that consists of a vortex signal that changes according to the flow rate, a vortex flowmeter signal amplification circuit with a notch filter whose natural frequency of the cantilever vortex detector is nu11 frequency Is provided.

実施例 第1図は、本考案を適用する一例としての渦流量計10の
流れ方向における断面図を示す構成図、第2図は第1図
のII部の拡大図で、図中、1は導管であり、図示しない
被測配管に挟持され、渦流量計10の本体をなすものであ
る。該導管1内には渦発生体2が断面の直径を軸として
圧設固着しており、軸上に中空室25が穿設されており、
該中空室25には導圧孔21,22,23,24が貫通している。渦
発生体2の中空室25には導管1の上部を面状に裁削した
取付座11に取付フランジ31により固着された可撓筒3が
隙間をもって挿入されている。更に、該可撓筒3内には
取付フランジ31上部に載置される形で他の取付フランジ
41により固着された固着柱4が挿入される。該固定柱4
の端部には流れに面した左右の側面に電極42,43が貼着
されていて、可撓筒3を他の共通電極とした静電容量を
形成している。電極42,43の導線44,45は、固定柱4内部
を挿通してプリアンプ6に導通される。プリアンプ6は
取付筒5により導管1に固設される。
Embodiment FIG. 1 is a configuration diagram showing a cross-sectional view in the flow direction of a vortex flowmeter 10 as an example to which the present invention is applied, and FIG. 2 is an enlarged view of a II portion of FIG. A conduit, which is sandwiched between pipes to be measured (not shown) and forms the main body of the vortex flowmeter 10. A vortex generator 2 is press-fitted and fixed in the conduit 1 with the diameter of the cross section as an axis, and a hollow chamber 25 is bored on the axis.
Pressure guiding holes 21, 22, 23, 24 penetrate through the hollow chamber 25. In the hollow chamber 25 of the vortex generator 2, a flexible cylinder 3 fixed by a mounting flange 31 to a mounting seat 11 formed by cutting the upper portion of the conduit 1 into a plane is inserted with a gap. Further, in the flexible cylinder 3, another mounting flange is mounted on the upper side of the mounting flange 31.
The fixed column 4 fixed by 41 is inserted. The fixed column 4
Electrodes 42 and 43 are attached to the left and right side surfaces facing the flow at the end of the, to form a capacitance using the flexible tube 3 as another common electrode. The lead wires 44, 45 of the electrodes 42, 43 are inserted into the fixed column 4 and electrically connected to the preamplifier 6. The preamplifier 6 is fixed to the conduit 1 by a mounting cylinder 5.

上述の渦流量計10は、渦発生体に伴って生ずる変動圧を
導圧孔21〜24を介して中空室25内に導入し、導入された
変動圧力を受けて片持式に固着された可撓筒3が変動す
る変位を固定柱4の電極42,43により静電容量の変化と
して検出するものである。
The above-mentioned vortex flowmeter 10 introduces the fluctuating pressure generated by the vortex generator into the hollow chamber 25 through the pressure guiding holes 21 to 24, and is fixed in a cantilever manner upon receiving the fluctuating pressure introduced. The changing displacement of the flexible cylinder 3 is detected by the electrodes 42 and 43 of the fixed column 4 as a change in electrostatic capacitance.

第3図はプリアンプ6のブロック図を示すもので、渦信
号Aからの信号は遮断周波数のfaの近似微分要素Bと遮
断周波数fbをもつ2次遅れ素子Cとをもった従来技術に
おける増幅特性をもち、対称形Twin−T回路Dに入力す
る。対称Twin−T回路は、周知のフィルタ回路であり、
抵抗Rと容量2CのT形回路と容量Cと抵抗R/2のT形回
路の並列T形回路で、その伝達関数T(S)は、 をもち、ヌル(null)周波数 に選ばれる。この周波数f0は可撓筒3が取付フランジ31
を支持部とした固有振動数であり、検出周波数f=0.33
f0までの検出が可能となり第4図の周波数特性が得られ
た。
FIG. 3 shows a block diagram of the preamplifier 6, in which the signal from the vortex signal A has an amplification characteristic in the prior art having an approximate differential element B of the cutoff frequency fa and a secondary delay element C having the cutoff frequency fb. Input to the symmetrical Twin-T circuit D. The symmetrical Twin-T circuit is a well-known filter circuit,
The transfer function T (S) is a parallel T-type circuit consisting of a T-type circuit with a resistor R and a capacitance 2C and a T-type circuit with a capacitance C and a resistor R / 2 With a null frequency To be chosen. At this frequency f 0, the flexible cylinder 3 has a mounting flange 31
Is the natural frequency with the support as the detection frequency f = 0.33
Detection up to f 0 is possible, and the frequency characteristics shown in Fig. 4 are obtained.

第5図及び第6図は、それぞれ第8図及び第9図に示し
た流量を等しい流量の583Hz(0.182f0)と1100Hz(0.34
4f0)における渦信号を示すもので、(a)図の周波数
成分図において可撓筒3の固有振動数のf0雑音成分が減
少しており、S/Nの改善が第8図及び第9図との比較に
おいてみられる。第3図Eの比較回路、Fの出力回路は
周知の回路であり、Out端子から渦パルス信号として出
力される。
Figures 5 and 6 show the flow rates shown in Figures 8 and 9, respectively, at the same flow rates of 583Hz (0.182f 0 ) and 1100Hz (0.34).
4f 0 ), the f 0 noise component of the natural frequency of the flexible cylinder 3 is reduced in the frequency component diagram of FIG. (A), and the improvement of S / N is shown in FIG. 8 and FIG. Seen in comparison with Figure 9. The comparison circuit of FIG. 3E and the output circuit of F are known circuits, and are output as eddy pulse signals from the Out terminal.

叙上の本考案のプリアンプは、渦検出方法において、前
述の特公昭63−31726号公報に開示され渦流量形にも適
用される。即ち、可撓筒3内に短冊上母材に歪検出素子
を固着してなる歪検出方式にもおいても、可撓筒3が取
付フランジ31を支持部とする片持ばり入固有振動数をも
っているので、該固有振動数が渦信号に雑音成分として
混入しS/Nを悪化させる。尚、叙上の方式以外において
も渦信号に検出要素における固有振動雑音が混入する場
合に適用できる。
The above-described preamplifier of the present invention is also applied to the vortex flow type disclosed in the above-mentioned Japanese Patent Publication No. 63-31726 in the vortex detection method. That is, even in the strain detection method in which the strain detecting element is fixed to the strip-shaped base material in the flexible cylinder 3, the cantilevered natural frequency of which the flexible cylinder 3 uses the mounting flange 31 as a support portion. Therefore, the natural frequency mixes in the vortex signal as a noise component and deteriorates the S / N. It should be noted that the method other than the above method can be applied when the natural vibration noise in the detection element is mixed in the vortex signal.

効果 以上の説明から明らかなように、本考案によれば、検出
要素に含まれる可撓筒の固有振動雑音f0が効果的に除去
され、従来検出可能な渦周波数fがf=0.2f0程度が限
界であったのに比し、f=0.4f0〜0.45f0の高域流量で
計測が可能である。しかも、対称Twin−T回路の簡単な
回路を付加することにより極めて効果のある特性が得ら
れる。
Effects As is apparent from the above description, according to the present invention, the natural vibration noise f 0 of the flexible cylinder included in the detection element is effectively removed, and the conventionally detectable vortex frequency f is f = 0.2f 0. In contrast to the limit of the degree, it is possible to measure at a high range flow rate of f = 0.4f 0 to 0.45f 0 . In addition, by adding a simple symmetrical Twin-T circuit, extremely effective characteristics can be obtained.

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

第1図は、本考案の渦流量計信号増幅回路を適用する渦
流量計の一例を示す構成図、第2図は第1図のII部拡大
図、第3図は信号増幅回路のブロック図、第4図は、周
波数特性を示す図、第5図及び第6図は、本考案の増幅
回路を用いた場合の渦信号を示す図、第7図は、従来技
術の周波数特性図、第8図及び第9図は、従来の増幅回
路を用いた場合の渦信号を示す図である。 1…導管,2…渦発生体,3…可撓筒,4…固定柱,6…プリア
ンプ,10…渦流量計。
FIG. 1 is a configuration diagram showing an example of a vortex flowmeter to which the vortex flowmeter signal amplification circuit of the present invention is applied, FIG. 2 is an enlarged view of a II portion of FIG. 1, and FIG. 3 is a block diagram of the signal amplification circuit. FIG. 4 is a diagram showing a frequency characteristic, FIGS. 5 and 6 are diagrams showing an eddy signal when the amplifier circuit of the present invention is used, and FIG. 7 is a frequency characteristic diagram of a conventional technique. FIG. 8 and FIG. 9 are diagrams showing vortex signals when a conventional amplifier circuit is used. 1 ... Conduit, 2 ... Vortex generator, 3 ... Flexible tube, 4 ... Fixed column, 6 ... Preamplifier, 10 ... Vortex flowmeter.

Claims (3)

【実用新案登録請求の範囲】[Scope of utility model registration request] 【請求項1】流体が流れる導管内に配設され、発生した
カルマン渦による変動圧力が導入される中空室を有する
渦発生体と、前記中空室内に挿入され前記渦発生体の一
端側に片持支持される可撓体と、前記変動圧力に応動し
て変位する前記可撓体の交番変位を検知する渦検出手段
と、該渦検出手段により検出された単位時間当りに発生
する渦の数により流量を求める信号増幅回路とからなる
渦流量計において、前記信号増幅回路に、前記渦検出手
段により検知された前記可撓体の交番変位信号を所定レ
ベルに増幅する増幅回路と、該増幅回路により増幅され
た信号に含まれる前記可撓体の固有振動数をヌル(Nu1
1)周波数とした対称ツイン(Twin)・Tフィルタ回路
とを有することを特徴とする渦流量計信号増幅回路。
1. A vortex generator having a hollow chamber, which is disposed in a conduit through which a fluid flows, and into which a fluctuating pressure due to a generated Karman vortex is introduced, and a vortex generator which is inserted into the hollow chamber and has one end on one side thereof. A flexible body that is held and supported, a vortex detection unit that detects an alternating displacement of the flexible body that is displaced in response to the fluctuating pressure, and the number of vortices generated per unit time detected by the vortex detection unit. In the vortex flowmeter, which comprises a signal amplification circuit for obtaining a flow rate by means of the signal amplification circuit, an amplification circuit for amplifying the alternating displacement signal of the flexible body detected by the vortex detection means to a predetermined level, and the amplification circuit. The natural frequency of the flexible body included in the signal amplified by
1) A vortex flowmeter signal amplification circuit characterized by having a symmetrical twin (Twin) / T filter circuit with a frequency.
【請求項2】前記渦発生体の前記中空室に挿入された可
撓体を可撓筒とし、該可撓筒の交番変位の検出手段を、
該可撓体を可動電極とし、該可撓筒内に挿入された固定
柱の側面に絶縁固着された固定電極とからなる静電検出
器としたことを特徴とする請求項1に記載の渦流量計信
号増幅回路。
2. A flexible cylinder inserted into the hollow chamber of the vortex generator is a flexible cylinder, and means for detecting an alternating displacement of the flexible cylinder is provided.
2. The vortex according to claim 1, wherein the flexible body is a movable electrode, and the electrostatic detector is composed of a fixed electrode that is insulated and fixed to a side surface of a fixed column inserted into the flexible cylinder. Flowmeter signal amplification circuit.
【請求項3】前記渦発生体の前記中空室に挿入された可
撓体を可撓筒とし、該可撓筒の交番変位の検出手段を、
該可撓体内に挿入され該可撓体の交番変位に応動する短
冊状母材に固着された歪検出素子としたことを特徴とす
る請求項1に記載の渦流量計信号増幅回路。
3. A flexible cylinder inserted into the hollow chamber of the vortex generator is a flexible cylinder, and means for detecting an alternating displacement of the flexible cylinder is provided.
The vortex flowmeter signal amplification circuit according to claim 1, wherein the strain detection element is a strain detection element that is inserted into the flexible body and fixed to a strip-shaped base material that responds to an alternating displacement of the flexible body.
JP1988148227U 1988-11-14 1988-11-14 Vortex flowmeter signal amplification circuit Expired - Lifetime JPH0648351Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1988148227U JPH0648351Y2 (en) 1988-11-14 1988-11-14 Vortex flowmeter signal amplification circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1988148227U JPH0648351Y2 (en) 1988-11-14 1988-11-14 Vortex flowmeter signal amplification circuit

Publications (2)

Publication Number Publication Date
JPH0269719U JPH0269719U (en) 1990-05-28
JPH0648351Y2 true JPH0648351Y2 (en) 1994-12-12

Family

ID=31419354

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1988148227U Expired - Lifetime JPH0648351Y2 (en) 1988-11-14 1988-11-14 Vortex flowmeter signal amplification circuit

Country Status (1)

Country Link
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Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58154620A (en) * 1981-12-10 1983-09-14 ザ・バブコツク・アンド・ウイルコツクス・カンパニ− Tunable notch filter for reducing sensitivity of vibration of vortex separating type flowmeter signal generator

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58154620A (en) * 1981-12-10 1983-09-14 ザ・バブコツク・アンド・ウイルコツクス・カンパニ− Tunable notch filter for reducing sensitivity of vibration of vortex separating type flowmeter signal generator

Also Published As

Publication number Publication date
JPH0269719U (en) 1990-05-28

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