JPS5838816A - Electromagnetic flowmeter - Google Patents

Electromagnetic flowmeter

Info

Publication number
JPS5838816A
JPS5838816A JP13708481A JP13708481A JPS5838816A JP S5838816 A JPS5838816 A JP S5838816A JP 13708481 A JP13708481 A JP 13708481A JP 13708481 A JP13708481 A JP 13708481A JP S5838816 A JPS5838816 A JP S5838816A
Authority
JP
Japan
Prior art keywords
converter
electromotive force
constant
signal electromotive
oscillator
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.)
Pending
Application number
JP13708481A
Other languages
Japanese (ja)
Inventor
Ichiu Suzuki
鈴木 一宇
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.)
Yokogawa Electric Corp
Original Assignee
Hokushin Electric Works Ltd
Yokogawa Hokushin Electric 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 Hokushin Electric Works Ltd, Yokogawa Hokushin Electric Corp filed Critical Hokushin Electric Works Ltd
Priority to JP13708481A priority Critical patent/JPS5838816A/en
Publication of JPS5838816A publication Critical patent/JPS5838816A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01FMEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
    • G01F1/00Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
    • G01F1/56Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using electric or magnetic effects
    • G01F1/58Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by using electric or magnetic effects by electromagnetic flowmeters
    • G01F1/60Circuits therefor

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Fluid Mechanics (AREA)
  • General Physics & Mathematics (AREA)
  • Measuring Volume Flow (AREA)

Abstract

PURPOSE:To obtain interchangeability between an oscillator and converter, by making the dispersion in a signal electromotive force generated on the oscillator side as a constant for the oscillator, and compensating for the signal electromotive force by said constant at the converter side. CONSTITUTION:The oscillatorIoutputs the signal electromotive force which is generated across electrodes 3 and 3a when fluid to be measured flows through the magnetic field formed by supplying an exciting current through an exciting coil 1. The intrinsic current K of the oscillatorIis expressed by K=ets/ess, where ess is the standard signal electromotive force of a standard oscillator and ets is signal electromotive force of the ordinary oscillatorIunder the same conditions. The full scale flow rate 1 is set in a flow rate setting part 15a of a setting part 15 in the converter II, and, at the same time, the intrinsic constant K of the oscillatorIwhich is combined to a meter setting part 15b is set in the meter setting part 15b. In the converter II, the signal electromotive force, which is inputted to the converter II from the oscillatorI, is multiplied or divided by the constant K and outputted. In this way, the interchangeability between the oscillator and the converter can be obtained.

Description

【発明の詳細な説明】 本実I14は電磁流量計に関し、発信器と変換器との互
換性上確保しえものである・ 電磁流量針は磁界に直角に導電性の#!体【流した1l
KtW間に発生する流速に対応する太きさの起電力を発
生させ、これによシ流量!渕定する九めのものであ少、
前記起電力を発生する発信器とこの発信器からの微弱な
流量信号を統−電61信号若しくはパルス列信号に変換
する変換器とによp構成される0こOと1変換器は精密
なダイヤル目盛と関連し九利得調整用の可愛抵抗器【有
しており、発信器側の出力特性が一定している場合、例
えば流速y−1111114のとき、出力電圧・−IJ
O悔マにをいてフルスパン流量が例えば100→匈から
120→麺に変って4その変換器出力は、例えばフルス
パン流量で4v等、同じ値で得られるようくして−る・
ところが変換I)0利得の調Ilが完全であっても、発
信器側の特性がそのけちつきのため変換器の1!求して
いる特性に一致してiないと変換器の出力信号Kit誤
差が會まれることとなる。そしてかかる発信器の特性の
ばらつきは例えばその製造時における口径のばらつき、
励−コイル01!数のばらつき及び#確コイル0*付状
態等によシ筒単に生起される。そζて従来技術KsPい
ては発慣器の特性のばらつき全励磁電流の調整で除去し
、その励磁電流値tIl&板等に表示しておくことによ
り両者の互換性を確保している。即ち、例えば基準とな
るV 寓1 mK+のとき発信器の出力信号が1 m 
Vとなるような励磁電流を各発信器毎に一定してこの励
磁電流値【銘板に衆記しておき、任意の変換器により発
m器に供給する励磁電流1m記励磁電流値に調整して両
者全組合せるようにし喪ものである・ ところがこのように励磁電流を1iillEする方式に
おいては、発信器は一定流速に対し一定の信号起電力を
発生するように設計しておか1に妙ればならず、乙のた
め微少口径の電磁流量針と大口径の電磁流量針の場合に
は必要なaim電流が大きくなル、消費電力O増加及び
IIJ碓回路の寸法、重量の増大ttE来してしまう、
これ#i藺看の場合には同じ磁束12Ffでは起電力鉱
口11に比例するという纏由によ9%また後者の場合に
は磁束91度は口径の2乗に比例するとiう履自による
からである・更に従来alfK>−ては励磁電流値を精
lIK設定する回路が必要とtkりそれだけ回路構成が
複JllKtらという欠点がある・本実I!AFi、上
記従来技術の欠点に鑑み、発信器の特性のばらつきに起
因する変換器の出力信号に対する影響を変換器側で除去
し両者の互換性上確保し得る電1m流量針を提供するこ
とを目的とする。そしてかかる目的音達成する本発明は
、発信器側で発生する信号起電力のばらつき【発信II
O定数として各発信器毎に一定しておき、この定数を変
換器に設定することによ)変換器側では前記信号起電力
の増幅率を変えるか若しくは信号起電力の大きさに前記
定数に比例した値t#4け合せるかして補正を行なうよ
うにした点tその技術思想の基礎とするものである・以
下本発明の実施例tri!JFIiK基づき詳細に説明
する。図に示すように、発信IW1は、励磁コイル1、
内sea定流体流体れる導管2及びこの導管2に装着さ
れ九電極3,3at有しており、定電1111114’
を有する励振回路厘よや励磁コイルIK励磁電#l管供
給して形成される磁界中【前記固定流体が流れたとき前
記電極3.3a間に発生する信号起電力!出力するもの
である・一方、変換器鳳は前記信号起電力管インピーダ
ンス変換するバッファアンプ5.6、このバッファアン
プ5.6の出力信号【増幅するプリアンプ7、ホールド
用のコンダンtC1とこれに蓄積された電荷を放電する
えめのスイッチ8W、Ili有し前記プリアンプ7の出
力信号tスイッチーwln断続によシサンプルして積分
する積分回路8゜フィードバック抵抗として可変抵抗1
) Rm會有して利得上調整し得るとともK11l記積
分1路$O出力信号を増幅する可変ゲインアンプ9及び
この可変ゲインアンプ9の出力信号tI&履し流量信号
として出力するマイクロコンピュータMOからな゛る・
j!に、マイクロコンビエータMOa、III記可変ゲ
インアンプ9の出力値ゑt−’/D変換するA/D責換
置換器10イクロプロセッサ11゜メモリ12.入出力
ボート13、このマイタロコンピュータMOて処置する
ディジタル信号tアナログ信号である流量信号に変換し
て出力するシム変換5114、スパンの設定を行なう流
量設定1i15aと発信器1に固有の定数を設定するメ
ータ定数設定1B1!!1)とt有する設定slB及び
これらの各機能ブロック関t−11絖しているデータバ
ス16とアドレスバス17からなシ、可変ゲインアンプ
90出力信号の処置の@K。
[Detailed Description of the Invention] This Act I14 relates to an electromagnetic flowmeter, and can be ensured in terms of compatibility between a transmitter and a converter. The electromagnetic flow needle has a conductive #! point perpendicular to the magnetic field. Body [1 liter flushed
Generates an electromotive force with a thickness corresponding to the flow velocity generated between KtW, and thereby increases the flow rate! This is the ninth thing that I have determined.
The 0 and 1 converters are composed of a transmitter that generates the electromotive force and a converter that converts the weak flow signal from the transmitter into a mains 61 signal or a pulse train signal. There is a resistor for gain adjustment associated with the scale, and if the output characteristics of the oscillator are constant, for example, when the flow rate is y-1111114, the output voltage -IJ
Unfortunately, if the full span flow rate changes from, for example, 100 to 120 to noodles, the converter output will be the same value, for example 4V at full span flow rate.
However, even if the conversion I) 0 gain key Il is perfect, the characteristics of the oscillator side are stingy and the converter's 1! If it does not match the desired characteristics, an error will occur in the output signal Kit of the converter. Variations in the characteristics of such transmitters include, for example, variations in diameter during manufacture,
Excitation coil 01! This may simply occur due to variations in the number of coils and the state of the #certain coil 0* attached. In the prior art KsP, the variation in the characteristics of the generator is removed by adjusting the total excitation current, and the excitation current value tIl is displayed on the plate, etc., thereby ensuring compatibility between the two. That is, for example, when the reference V is 1 mK+, the output signal of the oscillator is 1 m
Keep the excitation current constant for each transmitter and write it down on the nameplate, and adjust the excitation current to the excitation current value of 1m to be supplied to the generator using an arbitrary converter. However, in this method of increasing the excitation current, it would be a good idea to design the transmitter to generate a constant signal electromotive force for a constant flow velocity. However, in the case of a micro-diameter electromagnetic flow needle and a large-diameter electromagnetic flow needle, the required aim current increases, power consumption increases, and the size and weight of the IIJ Ususa circuit increase. Put it away,
In the case of #i, the same magnetic flux 12Ff is proportional to the electromotive force 11, which is 9%, and in the latter case, the magnetic flux 91 degrees is proportional to the square of the diameter. This is because the conventional alfK>- requires a circuit to precisely set the excitation current value, which has the drawback of requiring multiple circuit configurations. AFi, in view of the above-mentioned shortcomings of the prior art, aims to provide an electric 1m flow needle that can eliminate the influence on the output signal of the converter due to variations in the characteristics of the transmitter on the converter side and ensure compatibility between the two. purpose. The present invention that achieves such a target sound is characterized by variations in the signal electromotive force generated on the transmitter side [Transmission II
By setting this constant in the converter, the converter side can change the amplification factor of the signal electromotive force or adjust the magnitude of the signal electromotive force to the constant. The point that correction is performed by adding the proportional value t#4 is the basis of the technical idea.The following is an example of the present invention. This will be explained in detail based on JFIiK. As shown in the figure, the transmitting IW1 includes an exciting coil 1,
Inner sea constant fluid conduit 2 and this conduit 2 are equipped with nine electrodes 3, 3at, constant voltage 1111114'
In the magnetic field formed by supplying the excitation coil IK to the excitation circuit and the excitation tube, the signal electromotive force generated between the electrodes 3.3a when the fixed fluid flows! On the other hand, the converter Otori converts the signal electromotive force tube impedance into a buffer amplifier 5.6, the output signal of this buffer amplifier 5.6 [preamplifier 7 to amplify, condenser tC1 for holding, and accumulation in this] The output signal of the preamplifier 7 has a switch 8W and Ili for discharging the electric charge, and an integrating circuit 8 for sampling and integrating the output signal of the preamplifier 7 intermittently.A variable resistor 1 as a feedback resistor.
) A variable gain amplifier 9 which can adjust the gain by using Rm and amplifies the integral 1 path $O output signal described in K11l, and a microcomputer MO which outputs the output signal tI & output signal of this variable gain amplifier 9 as a flow rate signal. Nail・
j! , a micro combinator MOa, an A/D converter 10 for converting the output value of the variable gain amplifier 9 to t-'/D, a microprocessor 11, a memory 12. The input/output boat 13, the shim conversion 5114 that converts the digital signal t processed by this miterrocomputer MO into a flow rate signal which is an analog signal and outputs it, the flow rate setting 1i15a that sets the span, and constants specific to the transmitter 1 are set. Meter constant setting 1B1! ! 1) Setting slB and handling of the variable gain amplifier 90 output signal from the data bus 16 and address bus 17 connected to each of these functional blocks.

予め定められ大タイミングでスイッチ5vzsv*lW
m e lW4 @ Bah f断続スルトド4hII
c設定lll5に設定された数値に応じて可変ゲインア
ンプ会の11得t*mする。か(”Cスイツ? 814
 m B’Wm0III!によ〕励磁コイルIKは一定
の短y#波励磁電流が流れ、スイッチ8ux O断続に
よりプリアンプ70出力信号がサンプルされるとともに
前記スイッチ8W10逆の動作【行なうスイッチay、
の断続により電流検出抵抗りにより検出されアンプ18
で増@畜れ九定電流114からの負荷電流がサンプルさ
れる。j!に、スパンの設定は従来技術と同様に最大流
速として設定される一方、発信器1の固有の定数は標準
の発信器、即ち標準の励磁電at流したとき所定流速で
榔準の信号局電力管発生する発信@0定歓t」O・とし
てこれに対する比として表わされる・l1段tXに評言
すると、標準の発信器の標準の信号起電力を・、1とし
、一般O発4IiIs1の同条件での信号起電力【・t
−とすると、この発信IIIに固有の定IIR区罵・t
a/   とする。即ち、標準・−− の発信器が標準のjlIiIlIIE#1″′e流遮1
−/@@60とき1 sVの信号起電力を発生し九こと
を基準にし、一般の発信器1が同様のall電流で流速
lう4゜。のときLO3111V011号起電力!発生
しえとすると、この発信!110定数lc−In31/
1 = 11)1となる・ かかる電a#l量針において、変換器10出カーM(S
)、変換器1のスパン設定値(m速0フルスケール)轄
マ(gA#)、メータ設定11 (発信器IK崗有O定
数) −m K =m・ts/、、、、発信器I【実l
l1KfILれる調定流体O#1遣麿マ(ジ警)とする
と、 標準O発信器に訃ける流速マ(−和)のときの信号起電
力 ・、 &)  ■マ・1−1 一般の発信器IK訃ける流速マ(−騒)のときの信号起
電力 ・t(→■マ・t−となる。
Switch 5vzsv*lW at predetermined timing
m e lW4 @ Bah f intermittent sultodo 4hII
11 of the variable gain amplifier t*m according to the value set in c setting lll5. (“C Sweets? 814
m B'Wm0III! ] A constant short y# wave excitation current flows through the excitation coil IK, and the output signal of the preamplifier 70 is sampled by turning on and off the switch 8ux O, and the switch 8W10 reverses the operation.
It is detected by the current detection resistor due to the interruption of the amplifier 18.
The load current from the constant current 114 is sampled at . j! In this case, the span setting is set as the maximum flow velocity as in the prior art, while the specific constant of the transmitter 1 is the standard transmitter, i.e., the standard signal station power at a given flow rate when the standard excitation current is applied. The transmission generated by the tube is expressed as a ratio to this as ``O'', and the standard signal emf of a standard transmitter is . Signal electromotive force at [・t
-, then the specific IIR area specific to this transmission III is
a/. That is, the standard transmitter is the standard jlIiIlIIE#1'''e flow interrupter 1
-/@@60 When a signal electromotive force of 1 sV is generated, the general transmitter 1 has a flow rate of 4° with the same all current. When LO3111V011 electromotive force! If it happens, this message will be sent! 110 constant lc-In31/
1 = 11) 1. In such an electric a#l quantity needle, the converter 10 output car M(S
), span setting value of converter 1 (m speed 0 full scale) control ma (gA#), meter setting 11 (transmitter IK constant) -m K = m・ts/,,,, transmitter I [Real
If the regulated fluid O#1 is used as l1KfIL, then the signal electromotive force when the flow velocity is equal to the standard O transmitter (-sum) is... &) ■Ma 1-1 General transmission The signal electromotive force・t(→■ma・t−) when the flow velocity is low (-noise).

一方、変換器10出力mF1次式で与えられる・1m・
i/iv (但し・1sIIm入力値号)し九がって標
準の発信器と組合せ九ときの変換1sio出力罵は次の
過多である。
On the other hand, the converter 10 output mF is given by the linear equation ・1m・
i/iv (however, 1sIIm input value number) and the conversion 1sio output when combined with a standard oscillator is as follows.

M ” T、66g7. (”:、 K am l 、
 @1 #・−に)1マ・1−)・・・■ 一方、−1Rの発信器1と組合せたときの変換lll0
出力Mは次6jljでToる・11@、、、マ・・t+
I/@ts、y 3111 v、s51/v(a:、’
 ” @tll/、、、 、 @1 xm @@、 (
y) ■V・t@ )O・・■ 0式8@弐〇@呆【砿ぺれば両者が同値であることが1
lIIiされる。即ち、変換器1の設定部1sの流量設
定1g15aKフルスケールの流速を設定すると同時に
、メータ定数設定l115bにこれと組合せる発信器1
に固有の定数!を設定すれば両者の互換性がとれる・ なお、” −”i/x、v O演算は・10信号’t 
VD変換し丸後ディジタル演算する方法と、前記実施例
のように可変ゲインアンプ9の利得【マイクロコンピュ
ータMOの指令で変える方法とがあや、これはどちらで
4良い・えだ前者の場合は簡単ではあるが、VD変換l
Iのダイナミックレンジ管大きくする必lIがあ)、ま
え後者の場合は可変ゲインアンプ90ダイン設定の分解
能が必要とな9複雑になるという事実はある・以上実施
例とともに具体的に説明し良ように、事実WAKよれば
発信器側で発生する信号起電力Qばらつ11奮発信器0
5@数として各発信is*に測定してかき、こO定at
変換器に設定すゐことにより変換器側では前記信号起電
力の増幅率を変えるか若しくは信号起電力の大きさに前
記定数に比例した値會掛は合せるかして補正を行なうよ
うにし九〇で、変換器側のW/411で発信器との互換
性をとることができ、これに伴なう作業等が容易になる
M ” T, 66g7. (”:, Kam l,
@1 #・-に)1MA・1-)・・・■ On the other hand, the conversion lll0 when combined with -1R oscillator 1
The output M goes to the next 6jlj.・11@,,,Ma・・t+
I/@ts,y 3111 v,s51/v(a:,'
” @tll/,,, , @1 xm @@, (
y) ■V・t@ )O・・■ 0 formula 8 @ 2〇 @ 呆
lIIIi will be done. That is, at the same time, the flow rate setting 1g15aK of the setting unit 1s of the converter 1 is set to the full scale flow rate, and the transmitter 1 combined with this is set to the meter constant setting 115b.
A constant specific to ! You can make both compatible by setting ・In addition, "-"i/x, v O operation is ・10 signals 't
There is a difference between the method of performing VD conversion and digital calculation after rounding, and the method of changing the gain of the variable gain amplifier 9 [by command of the microcomputer MO] as in the above embodiment. However, VD conversion
However, in the latter case, the resolution of the variable gain amplifier's 90-dyne setting is required, which makes it more complicated.Let's explain this in detail with the above examples. In fact, according to WAK, the signal electromotive force Q variation generated on the transmitter side is 11 and the transmitter is 0.
5@Measure each outgoing is* as a number and write this O constant at
By setting it in the converter, the converter side can perform correction by changing the amplification factor of the signal electromotive force or by matching the magnitude of the signal electromotive force with a value proportional to the constant. Therefore, the W/411 on the converter side can be compatible with the transmitter, and the associated work etc. can be facilitated.

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

図は電磁流量計を示すプロッタ線図・ 図  閾  中、 1線発信器、 1は変換器、 15tj設定部、 15bFiメ一タ定数設定部である。 特許出願人 株式会社北辰電機製作所 代   理   人 弁麿士党石士部 (m1名) The figure is a plotter diagram showing an electromagnetic flowmeter. In Figure Threshold, 1 line transmitter, 1 is a converter, 15tj setting section, 15bFi meter constant setting section. patent applicant Hokushin Electric Manufacturing Co., Ltd. Representative person Benmaroshi Party Ishishi Club (m1 people)

Claims (1)

【特許請求の範囲】[Claims] 発信器と変換器とt有し、且つ発信器の励磁コイルKt
j定電流が供給される電磁流量計において、標準の励磁
電流と所定OIl速において標準の発@器が発生する信
号起電力と、同様0条件で前記発信器が発生する信号起
電力との比をその発信!Kll有の定数とし、前記変換
器において前記定数を設定し前記発信器から前記変換量
に入力される信号起電力に前記定数を乗算若しくけ除算
して出力するようにしたこと141黴とする電磁流量針
It has a transmitter, a converter, and an excitation coil Kt of the transmitter.
jIn an electromagnetic flowmeter to which a constant current is supplied, the ratio of the signal electromotive force generated by a standard generator at a standard excitation current and a predetermined oil speed to the signal electromotive force generated by the transmitter under the same zero condition. That message! Kll is a constant, and the constant is set in the converter, and the signal electromotive force input from the oscillator to the conversion amount is multiplied or divided by the constant and outputted. Electromagnetic flow needle.
JP13708481A 1981-09-02 1981-09-02 Electromagnetic flowmeter Pending JPS5838816A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13708481A JPS5838816A (en) 1981-09-02 1981-09-02 Electromagnetic flowmeter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13708481A JPS5838816A (en) 1981-09-02 1981-09-02 Electromagnetic flowmeter

Publications (1)

Publication Number Publication Date
JPS5838816A true JPS5838816A (en) 1983-03-07

Family

ID=15190509

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13708481A Pending JPS5838816A (en) 1981-09-02 1981-09-02 Electromagnetic flowmeter

Country Status (1)

Country Link
JP (1) JPS5838816A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010539512A (en) * 2007-09-18 2010-12-16 ローズマウント インコーポレイテッド General-purpose transmitter for electromagnetic flowmeter

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010539512A (en) * 2007-09-18 2010-12-16 ローズマウント インコーポレイテッド General-purpose transmitter for electromagnetic flowmeter

Similar Documents

Publication Publication Date Title
JPS5838816A (en) Electromagnetic flowmeter
KR940000943B1 (en) Law level vtg pulse converter
CN208638250U (en) A kind of power supply system of excitation coil-moving speaker
JPH07324959A (en) Electromagnetic flowmeter
EP0062531B2 (en) Electromagnetic flow meter
JP2946156B2 (en) Electromagnetic flow meter
JPS5929279Y2 (en) Gain switching device in flow signal transmission device
KR960039606A (en) Amplitude adjustment circuit and method thereof
JPS606733Y2 (en) Flowmeter output processing circuit
JPH08146050A (en) Measuring instrument using differential amplifier
JPH08285646A (en) Integral electromagnetic flow meter
JPH0552560B2 (en)
CN108649790A (en) A kind of power supply system of excitation coil-moving speaker
JP2893364B2 (en) Electromagnetic flow meter
JP3175569B2 (en) Bus system power supply
JPS61107178A (en) Method and apparatus for receiving pulse signal wave
JPS6225718Y2 (en)
JPS5997430U (en) electromagnetic flow meter
SU696292A1 (en) Rate-of-flow meter
SU1374144A1 (en) Digital conductivity apparatus
JPS6318197Y2 (en)
JPH07209049A (en) Two wire system electromagnetic flow meter
JPS63314941A (en) Automatic power measuring method for analog signal
JPH0821754A (en) Two-wire type electromagnetic flowmeter
JPS6022798B2 (en) 2-wire signal converter