JPS5824813A - Exciting circuit for electromagnetic flowmeter - Google Patents

Exciting circuit for electromagnetic flowmeter

Info

Publication number
JPS5824813A
JPS5824813A JP12320881A JP12320881A JPS5824813A JP S5824813 A JPS5824813 A JP S5824813A JP 12320881 A JP12320881 A JP 12320881A JP 12320881 A JP12320881 A JP 12320881A JP S5824813 A JPS5824813 A JP S5824813A
Authority
JP
Japan
Prior art keywords
circuit
excitation
current
reference voltage
voltage signal
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
JP12320881A
Other languages
Japanese (ja)
Inventor
Toru Fujii
徹 藤井
Akira Sato
明 佐藤
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 JP12320881A priority Critical patent/JPS5824813A/en
Publication of JPS5824813A publication Critical patent/JPS5824813A/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

Abstract

PURPOSE:To use one exciting circuit in common for current driving and voltage driving, by connecting voltage driving rectifier to a circuit comprising a diode bridge, a reference voltage signal generating circuit, an amplifier, and an active element, through circuit switching elements. CONSTITUTION:When only a switch J3 of switches J1-J7 is turned OFF, a current driving type exciting circuit is formed, and an exciting coil L is driven by the current through terminals Ix1 and Ix2. In the meantime, when only the circuit switch J3 is turned ON, capacitors C1 and C2, a diode D2 for protecting a reverse voltage, and a current limiting element Q2 are excluded from the circuit constitution, and the voltage driving rectifier 2 is incorporated into the circuit. Thus a voltage driving type exciting circuit is formed. Then the exciting coil L is driven by the voltage through output terminals Ex1 and Ex2 of the rectifier 2.

Description

【発明の詳細な説明】 本発明は電磁流i゛計の発信器を駆動する励振回路に関
し、特に、電流駆動と電圧駆動の両方を可能とした励振
回路に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an excitation circuit for driving an oscillator of an electromagnetic current meter, and more particularly to an excitation circuit capable of both current drive and voltage drive.

従来の電磁流量計には、励磁電流を変換器内にて電圧源
より作りこれを発信器の励磁コイルに流すと共に励磁電
流に比例した信号即ち比較信号で流量信号を除算するこ
とによQ励磁電流の変動に基づく出力誤差を除去すると
いう電圧励振方式と、変換器内にて定電流源で励磁電流
を作ることにより負荷にかかわらず一定振幅の励磁電流
を発信器の励磁コイルに流すという電流励振方式とがあ
る。前者の励振方式は比較信号をとるため電磁流量計の
発信器と変換器間に完全互換性があるという利点がある
。この利点は後者の励振方式には無く、メータファクタ
を発信器毎に設定する不便はあるが、比較信号回路が不
要であるから発信器と変換器間の結合が自由であるとい
う利点がある。
In conventional electromagnetic flowmeters, an excitation current is generated from a voltage source in a converter, and the current is passed through an excitation coil of a transmitter, and the flow rate signal is divided by a signal proportional to the excitation current, that is, a comparison signal. The voltage excitation method eliminates output errors due to current fluctuations, and the current method uses a constant current source to generate an excitation current within the converter, allowing a constant amplitude excitation current to flow through the excitation coil of the transmitter regardless of the load. There is an excitation method. The former excitation method has the advantage of being completely compatible with the transmitter and converter of the electromagnetic flowmeter since it takes a comparison signal. This advantage does not exist in the latter excitation method, and although there is the inconvenience of setting the meter factor for each oscillator, there is an advantage that the oscillator and converter can be freely coupled because a comparison signal circuit is not required.

そこで上記2種の励振方式の電磁流量計が既に多数用い
られているが、その変換器内の励振回路は励振方式に基
づいて電圧駆動と電流駆動という全く別の専用回路とな
っている。
Therefore, many electromagnetic flowmeters using the two types of excitation methods described above are already in use, but the excitation circuits in the converters are completely different dedicated circuits, one for voltage drive and one for current drive, based on the excitation method.

しかし、今後の励振回路は電圧駆動と電流駆動のいずれ
にも適合できる回路であることが望ましい。しかも回路
を構成する要素の多くを電圧駆動と電流駆動の両者に共
用できることが望ましい。
However, it is desirable that future excitation circuits be compatible with both voltage drive and current drive. Furthermore, it is desirable that many of the elements constituting the circuit can be used in common for both voltage drive and current drive.

本発明は上記要望に応えた電磁流量計励振回路を提供す
ることを目的とする。
An object of the present invention is to provide an electromagnetic flowmeter excitation circuit that meets the above-mentioned needs.

まず、第1〜4図を参照して本発明の詳細な説明してお
く。第1凸は従来から有る電圧駆動形の励振回路を示し
、商用電源1に対しスイッチSWを第2図(a)のタイ
ミングでオン・オフすると、ダイオードグリッジ2への
電源ライン間には同図(b)の電圧波形が表われ、励磁
コイルLには同図(e)の如く全波整流された電圧が印
加される。このスイッチSWは交流をオン・オフするた
めサイリスタが用いられ、オン・オフのタイミングは変
換器のタイミング回路3から与えられる。なお第1図中
、4は比較信号Vrefを作る回路であり、4aは整流
入力電流を検出するカレントトランス、4bと4cは励
磁コイルの持続電流を検出するダイオードとカレントト
ランス、4dは両カレントトランス4a、4aの出力を
合成・整流する整流器、4eは終端抵抗である。
First, the present invention will be explained in detail with reference to FIGS. 1 to 4. The first protrusion shows a conventional voltage-driven excitation circuit, and when the switch SW is turned on and off with respect to the commercial power supply 1 at the timing shown in Fig. 2(a), the power supply line to the diode grid 2 is connected between the power lines shown in Fig. 2(a). A voltage waveform shown in (b) appears, and a full-wave rectified voltage is applied to the excitation coil L as shown in (e) of the same figure. This switch SW uses a thyristor to turn on and off the alternating current, and the on/off timing is given from the timing circuit 3 of the converter. In Figure 1, 4 is a circuit that generates the comparison signal Vref, 4a is a current transformer that detects the rectified input current, 4b and 4c are diodes and current transformers that detect the continuous current of the excitation coil, and 4d is both current transformers. 4a is a rectifier that combines and rectifies the outputs of 4a, and 4e is a terminating resistor.

一方、第3図は*a昭56−10107号として出願し
た発明による電流駆動形の励振回路を示し、電源トラン
ス5、ダイオードグリッジ6及び平滑用コンデンサCI
、c!で直流電圧源を作シ、コンブリメンタリカ2つの
能動素子である1電流制限素子Qs=Qい増幅器Q3、
負帰還用の電流検出抵抗Rref  及び励磁電流に相
似な波形を持つ基準電圧信号の発生回路7でなる定電流
回路で励磁コイルLを電流駆動する。つまり、第4図(
a)に示す基準電圧信号の十Eの電圧が増幅器Q、の非
反転入力端子に加わると、Qlは能動領域でQ、がオフ
となって励磁コイルLにはQ1→Rref→Lの順で励
磁電流Iexが流れる。また−Eの電圧が増幅器Q3の
非反転入力端子に加わると、Qlが能動領域でQ、がオ
フとなってL→Rref−+Q1の順で励磁電流Iex
が流れる。このとき、抵抗Rref  の検出電圧Rr
e? Iexが増幅器Q3の反転入力端子に印加されて
いるため、Rref・Iex == Eと平衡するよう
にQl 、Qtの電流制限素子が増幅器Q、によシ制御
され、その結果第4図(b)に示すような電流駆動の励
磁電流が流れる。
On the other hand, Fig. 3 shows a current drive type excitation circuit according to the invention filed as *a No. 10107/1982, which includes a power transformer 5, a diode glitch 6, and a smoothing capacitor CI.
,c! A DC voltage source is created by combining two active elements, one current-limiting element Qs=Q, and an amplifier Q3,
The excitation coil L is current-driven by a constant current circuit comprising a current detection resistor Rref for negative feedback and a reference voltage signal generation circuit 7 having a waveform similar to the excitation current. In other words, Figure 4 (
When a voltage of 10E of the reference voltage signal shown in a) is applied to the non-inverting input terminal of the amplifier Q, Ql is in the active region and Q is turned off, and the excitation coil L is supplied in the order of Q1 → Rref → L. Excitation current Iex flows. Furthermore, when a voltage of -E is applied to the non-inverting input terminal of amplifier Q3, Ql is in the active region and Q is turned off, and the excitation current Iex is increased in the order of L→Rref-+Q1.
flows. At this time, the detection voltage Rr of the resistor Rref
e? Since Iex is applied to the inverting input terminal of amplifier Q3, the current limiting elements of Ql and Qt are controlled by amplifier Q so as to balance Rref·Iex == E, and as a result, as shown in FIG. ) A current-driven excitation current flows as shown in ().

励磁電流の値は抵抗値Rref または基準電圧信号の
振幅Eを変えることにより、制御される。
The value of the excitation current is controlled by changing the resistance value Rref or the amplitude E of the reference voltage signal.

そこで、第1図と第3図の回路を比較検討したところ、 (1)第3図のダイオードグリッジ6と電流制限素子Q
1又はQ2を組合せることによp第1図のスイッチSW
に相当する交流スイッチを構成でき、このことから、電
流制限素子をオン・オフ動作させると共にコンデンサC
,、C,等の不要な部品を除き、且つ第1図のダイオー
ドブリッジ2に相当する整流器を追加すれば電圧駆動形
の励振回路に変更できること、(2)一方、第3図にお
いて2つの電流制限素子Q、、Q、lをオン・オフ動作
させ且つコンデンサC,,C,を除き、抵抗Rrefま
たは基準電圧信号の振幅Eを変えるだけでも電圧駆動形
の励振回路に変更できること、 が判明した。
Therefore, after comparing and examining the circuits in Figures 1 and 3, we found that: (1) Diode glitch 6 and current limiting element Q in Figure 3.
1 or Q2 in combination, the switch SW in Figure 1
It is possible to configure an AC switch corresponding to
, C, etc., and by adding a rectifier corresponding to the diode bridge 2 in Fig. 1, it is possible to change it to a voltage-driven excitation circuit. (2) On the other hand, in Fig. 3, the two currents It has been found that it is possible to change the excitation circuit to a voltage-driven type by simply turning on and off the limiting elements Q, Q, and l, removing the capacitors C, and C, and changing the resistor Rref or the amplitude E of the reference voltage signal. .

以下、第5〜IC図に基づいて本発明の詳細な説明する
。なお、各図で第1,3図と同機能のものは同符号を付
して説明の重複を省く。
Hereinafter, the present invention will be described in detail based on FIGS. In each figure, parts having the same functions as those in FIGS. 1 and 3 are given the same reference numerals to avoid redundant explanation.

第5図は本発明の一実施例を示し、占〜J7は回路切換
用のスイッチであシ、各スイッチJ1〜J、を図示の状
態即ち、J3だけオフとすれば第3図と等価な電流駆動
形の励振回路となってエエ、。
FIG. 5 shows an embodiment of the present invention, where J7 to J7 are switches for switching circuits, and if each switch J1 to J is in the state shown, that is, only J3 is turned off, the result is equivalent to that in FIG. It becomes a current drive type excitation circuit.

Ix2の端子を通じて励磁コイルLを電流駆動できる。The exciting coil L can be driven with current through the terminal Ix2.

一方、J、の回路切換スイッチだけをオンとすればコン
デンサC,,C,、D、とり、のうち一方の逆電圧保護
用のダイオ−t’Dt及びQ、とQ2のうち一方の電流
制限素子Q2が回路構成から外れ、逆に電圧駆動用の整
流器2が回路に入る。この状態を第6図に示す。第6図
中のダイオードグリッジ6とその+、一端子間に入った
電流制限素子Q1とがなす回路を等測的に表わすと第7
図にな!0、Q、のオン・オフを表わすスイッチSW。
On the other hand, if only the circuit changeover switch J is turned on, the reverse voltage protection diode t'Dt of one of the capacitors C, , C, , D, and the current limit of one of Q and Q2 Element Q2 is removed from the circuit configuration, and conversely, voltage-driven rectifier 2 is inserted into the circuit. This state is shown in FIG. The circuit formed by the diode glitch 6 in FIG. 6 and the current limiting element Q1 inserted between its + and one terminal is expressed isometrically as
Illustrated! Switch SW that indicates on/off of 0 and Q.

のオン・オフによfiA−B間がオン・オフする交流ス
イッチが構成される。この場合スイッチSW2を流れる
電流は一方向であるから、Qlとしてはトランジスタや
MOS−FET?l:どの半導体能動素子を用いること
ができる。また、Q、をスイッチング素子として能動領
域外でオン・オフさせるには基準電圧信号の発生口wr
I中のポテンショメータVRにより基準電圧信号の振幅
Eを大きくすれば良い。々お、7の回路中、ZDはゼナ
ーダイオード、SW、、とSW、−2Bはタイミング回
路3からの信号によシ交互に開閉するスイッチである。
An alternating current switch is configured to turn on and off between fiA and B. In this case, the current flowing through switch SW2 is unidirectional, so Ql should be a transistor or MOS-FET? l: Any semiconductor active device can be used. In addition, in order to turn on and off Q as a switching element outside the active region, the reference voltage signal generation port wr
The amplitude E of the reference voltage signal may be increased using the potentiometer VR in I. In the circuit 7, ZD is a zener diode, SW, .

したがって、第6図の回路は第1図と等価な電圧駆動形
の励振回路とな夛、整流器2の出力端子EX” +胸2
を通じて励磁コイルLを電圧駆動できる。なお、電流検
出用の抵抗Rrefは外してもかまわりいが、図の如く
残しRref・Iex(Eとしておくと、出力端子EX
I、EX2短絡時の過大電流に対し電流リミッタとして
働く。つまシ、抵抗Rrefに発生する電圧が一定値を
越えるとQ、が能動領域に入って電流を制限する。更に
、電圧駆動の際は第6図中に破線で示す如くスイッチJ
、、J、でトランス5をバイパスさせても良い。
Therefore, the circuit in FIG. 6 is a voltage-driven excitation circuit equivalent to that in FIG.
The excitation coil L can be driven with voltage through. Note that you can remove the current detection resistor Rref, but if you leave it as Rref・Iex (E) as shown in the figure, the output terminal EX
Acts as a current limiter against excessive current when I and EX2 are short-circuited. When the voltage generated across resistor Rref exceeds a certain value, Q enters the active region and limits the current. Furthermore, when driving with voltage, switch J is connected as shown by the broken line in FIG.
,,J, may be used to bypass the transformer 5.

第8図は他の実施例を示す。この実施例では、電圧駆動
と電流駆動いずれでも励磁コイルLを電源トランス5と
一対の電流制限菓子Q1−Q20両中位点間、つまシ第
5図におけるIxl 、 IX2間に接続し、電圧駆動
の際には回路切換スイッチJ、。、J、1をオフにして
コンデンサC,、C,を切離す。JIOと511をオン
にすれば第5図と全く同じ電流駆動の励振回路となる。
FIG. 8 shows another embodiment. In this embodiment, in both voltage drive and current drive, the excitation coil L is connected between the power transformer 5 and the midpoints of the pair of current limiters Q1-Q20, and between Ixl and IX2 in FIG. In this case, use the circuit changeover switch J. , J,1 is turned off to disconnect the capacitor C,,C,. If JIO and 511 are turned on, it becomes a current-driven excitation circuit exactly the same as that shown in FIG.

一方、JIGと41をオフにしまた第6図と同じく電流
制限素子Qt +Q2をオン、オフ動作させれば励磁コ
イルLには第9図に示すような正・負の電圧が印加され
て全波の電圧駆動となる。またこの実施例の場合も、電
流検出用の抵抗Rrefを残しRref・Iex (E
としておくと電圧駆動時の過電流を制限できる。なお、
CTは比較信号Vref ’e得るためのカレントトラ
ンスであり、電流駆動の際はスイッチJl!+J1mで
これをバイパスすると良い。
On the other hand, if JIG and 41 are turned off and the current limiting element Qt +Q2 is turned on and off as shown in Fig. 6, positive and negative voltages as shown in Fig. 9 are applied to the exciting coil L, resulting in a full wave. It is driven by voltage. Also in this embodiment, the resistor Rref for current detection is left and Rref・Iex (E
By setting it as , it is possible to limit overcurrent during voltage drive. In addition,
CT is a current transformer for obtaining a comparison signal Vref 'e, and when driving with current, switch Jl! It is best to bypass this with +J1m.

第8図の実施例の場合、比較信号Vref  の作成は
同図の回路例の他、第10図(a)や伽)の回路によっ
ても行える。なお、K10図(a) 、 (b)には要
部だけを示し、ダイオードグリッジ6の出力側回路部分
は第8図と同じなので省略した。つまり、第10図(a
)の回路では、第8図と同じ接続のカレントトランスC
Tの出力を第1図と同様にグリッジ接続の整流器4dで
整流して比較信号Vrefとする。一方策10図(b)
の回路では、電源トランス5の二次中点間にカレントト
ランスCTの一次側を接続する。そしてカレントトラン
スCTの一次中点に励磁コイルLの一端を接続すると共
にカレントトランスCTの出力を整流器4dで整流して
比較信号Vref  としている。
In the case of the embodiment shown in FIG. 8, the comparison signal Vref can be generated by the circuit shown in FIG. Note that FIGS. K10 (a) and (b) show only the main parts, and the output side circuit part of the diode glitch 6 is omitted because it is the same as in FIG. 8. In other words, Fig. 10 (a
), the current transformer C with the same connection as in Fig.
The output of T is rectified by a glitch-connected rectifier 4d in the same manner as in FIG. 1 to provide a comparison signal Vref. Figure 10 (b)
In this circuit, the primary side of the current transformer CT is connected between the secondary midpoints of the power transformer 5. One end of the exciting coil L is connected to the primary center point of the current transformer CT, and the output of the current transformer CT is rectified by a rectifier 4d to provide a comparison signal Vref.

なお、上記各実施例では回路切換要素としてスイッチを
用いているが、これはジャンパ線による接続の有無等に
よっても良い。
In each of the embodiments described above, a switch is used as a circuit switching element, but this may be changed depending on whether or not a jumper wire is connected.

以上説明したように、本発明によれば電流駆動と電圧駆
動に一つの励振回路を共用できる。
As explained above, according to the present invention, one excitation circuit can be used in common for current drive and voltage drive.

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

第1,3図は本発明の原理説明用の回路図、第2,4図
はその波形図である。第5図は本発1 明の一実施例の回路図、第6図は第5図の回路を電圧駆
動用に切換えた場合の回路図、第7図は交流スイッチの
等価回路図、第8図は他の実施例の回路図、第9図は第
8図の電圧駆動時の波形図、第10図(a) 、 (b
)は第8図における比較信号作成の他の例を示す回路図
である。 図面中、 Lは励磁コイル 1は商用電源 2は電圧駆動用の整流器 5は電源トランス 6はダイオードグリッジ 7は基準電圧信号の発生回路 C1とC2はコンデンサ Q、とQ、は能rMJ累子 Q3は増幅器 J、〜J、3は回路切換スイッチである。 特許出願人  株式会社北辰電機製作所代 理 人  
弁理士光石士部(他1名)2 第10図 6 (b) re f 67−
1 and 3 are circuit diagrams for explaining the principle of the present invention, and FIGS. 2 and 4 are waveform diagrams thereof. Figure 5 is a circuit diagram of one embodiment of the first invention of the present invention, Figure 6 is a circuit diagram when the circuit in Figure 5 is switched to voltage drive, Figure 7 is an equivalent circuit diagram of an AC switch, and Figure 8 is an equivalent circuit diagram of an AC switch. The figure is a circuit diagram of another embodiment, Figure 9 is a waveform diagram during voltage drive in Figure 8, and Figures 10 (a) and (b).
) is a circuit diagram showing another example of comparison signal creation in FIG. 8; In the drawing, L is the excitation coil 1, the commercial power supply 2 is the voltage drive rectifier 5, the power transformer 6 is the diode grid 7 is the reference voltage signal generation circuit, C1 and C2 are the capacitors Q, and Q are the capacitors Q3. are amplifiers J, ~J, and 3 are circuit changeover switches. Patent applicant: Hokushin Electric Manufacturing Co., Ltd. Agent
Patent Attorney Mitsuishi Shibu (1 other person) 2 Figure 10 6 (b) ref 67-

Claims (2)

【特許請求の範囲】[Claims] (1)電磁流量計の励磁コイルへ流す励磁電流を交流電
源から作る励振回路において、ダイオードグリッジと、
平滑回路と、基準電圧信号の発生回路と、基準電圧信号
を増幅する増幅器と、この増幅器の出力信号により負荷
電流を制御する能wJ累子と、負荷電流を検出して前記
増幅器に負帰還をかける抵抗と、電圧駆動用整流器と、
回路切換要素とを備えてお9、前記ダイオ−Pグリッジ
で交流電力を整流しこれの平滑出力を前記能動素子で基
準電圧信号に応じた値の電流に制御して励磁コイルに流
す構成の励振回路と、この励振回路を構成する回路要素
のうちダイオードグリッジ、基準電圧信号の発生回路、
増幅器及び能動素子が共用され、このダイオードグリッ
ジの出力端子間に能m素子を接続して基準電圧信号に応
じて開閉する交流スイッチとしこの交流スイッチを介し
た交流電力を前記電圧駆動用整流器で整流して励磁コイ
ルに流す構成の励振回路とを、前記回路切換要素で選択
できる構成としたことを特徴とする電磁流量計励振回路
(1) In an excitation circuit that generates an excitation current from an AC power source to flow into an excitation coil of an electromagnetic flowmeter, a diode glitch is used.
A smoothing circuit, a reference voltage signal generation circuit, an amplifier that amplifies the reference voltage signal, a function wJ regulator that controls the load current using the output signal of this amplifier, and a load current that is detected and provides negative feedback to the amplifier. the resistor to be applied, the voltage-driven rectifier,
9, an excitation device configured to rectify alternating current power by the diode-P glitch, control its smoothed output to a current having a value according to a reference voltage signal by the active element, and send the current to the excitation coil. circuit, and among the circuit elements that make up this excitation circuit, a diode glitch, a reference voltage signal generation circuit,
An amplifier and an active element are shared, and an active element is connected between the output terminals of this diode glitch to create an AC switch that opens and closes in response to a reference voltage signal, and the AC power that has passed through this AC switch is rectified by the voltage drive rectifier. An excitation circuit for an electromagnetic flowmeter, characterized in that the excitation circuit configured to cause the current to flow through the excitation coil can be selected by the circuit switching element.
(2)  上記能動素子はブツシュゾル動作の一対の能
動素子でちゃ、そのうちの一つの能動素子が交流スイッ
チの構成に共用されることを特徴とする特許請求の範囲
第1項記載の電磁流量計励振回路。 (31’it磁流量計の励磁コイルへ流す励磁電流を交
流電源から作る励振回路に訃いて、交流電力を整流する
ダイオードグリッジと、平滑回路と、基準電圧信号の発
生回路と、基準電圧信号を増幅する増幅器と、この増幅
器の出力信号により負荷電流を制御するブツシュゾル動
作の一対の能動素子と、負荷電流を検出して前記増幅器
に負帰還をかける抵抗と、回路切換要素とを備えると共
に、励磁コイルは交流電源と前記一対の能動素子の各中
位点間に接続されるものとし、前記ダイオードグリッジ
と平滑回路からの整流平滑出力を前記一対の能動素子で
基準電圧信号に応じた値の電流に制御して励磁コイルに
流す構成の励振回路と、この励振回路を構成する回路要
素のうちダイオードグリッジ、基準電圧信号の発生回路
、増幅器及び一対の能動素子が共用され、このダイオー
ドグリッジの整流出力を基準電圧信号に応じた前記一対
の能動素子の開閉で励磁コイルに流す構成の励振回路と
を、前記回路切換要素で選択できる構成としたことを特
徴とする電磁流量計励振回路。
(2) The electromagnetic flowmeter excitation according to claim 1, wherein the active element is a pair of active elements that operate in a bush-sol manner, and one of the active elements is shared in the configuration of an AC switch. circuit. (In addition to the excitation circuit that generates the excitation current from the AC power supply to flow into the excitation coil of the 31'it magnetic flowmeter, it also includes a diode grid that rectifies the AC power, a smoothing circuit, a reference voltage signal generation circuit, and a reference voltage signal generation circuit. It includes an amplifier for amplification, a pair of active elements of Bushsol operation for controlling the load current by the output signal of the amplifier, a resistor for detecting the load current and applying negative feedback to the amplifier, and a circuit switching element. The coil is connected between the alternating current power supply and each midpoint of the pair of active elements, and the rectified and smoothed output from the diode glitch and smoothing circuit is used to generate a current of a value corresponding to the reference voltage signal in the pair of active elements. Among the circuit elements that make up this excitation circuit, a diode glitch, a reference voltage signal generation circuit, an amplifier, and a pair of active elements are shared, and the rectified output of this diode glitch is An excitation circuit for an electromagnetic flowmeter, characterized in that an excitation circuit configured to cause a current to flow through an excitation coil by opening and closing the pair of active elements according to a reference voltage signal can be selected by the circuit switching element.
JP12320881A 1981-08-06 1981-08-06 Exciting circuit for electromagnetic flowmeter Pending JPS5824813A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12320881A JPS5824813A (en) 1981-08-06 1981-08-06 Exciting circuit for electromagnetic flowmeter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12320881A JPS5824813A (en) 1981-08-06 1981-08-06 Exciting circuit for electromagnetic flowmeter

Publications (1)

Publication Number Publication Date
JPS5824813A true JPS5824813A (en) 1983-02-14

Family

ID=14854867

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12320881A Pending JPS5824813A (en) 1981-08-06 1981-08-06 Exciting circuit for electromagnetic flowmeter

Country Status (1)

Country Link
JP (1) JPS5824813A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112229457A (en) * 2020-11-19 2021-01-15 吉林大学 Novel electromagnetic flowmeter and measuring method thereof

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN112229457A (en) * 2020-11-19 2021-01-15 吉林大学 Novel electromagnetic flowmeter and measuring method thereof
CN112229457B (en) * 2020-11-19 2021-09-21 吉林大学 Novel electromagnetic flowmeter and measuring method thereof

Similar Documents

Publication Publication Date Title
US6381152B1 (en) Method of driving semiconductor switching device in non-saturated state and power supply apparatus containing such a switching device
JP3561876B2 (en) Variable output voltage power supply
JPS5824813A (en) Exciting circuit for electromagnetic flowmeter
JPH08289468A (en) Dc power supply for parallel operation
JP2533774Y2 (en) DC-DC converter
JPH01295670A (en) Overcurrent protective circuit
JPS63287364A (en) Auxiliary power circuit for switching regulator
JPH02133067A (en) Switching power supply
JP2686070B2 (en) Neutral wire open phase detection circuit breaker
JPS614416A (en) Overcurrent detector for switching power source
JPS5950772A (en) Power source
JPS6387173A (en) Power unit
JP2513741Y2 (en) Overcurrent detection circuit for switching power supply
JP2686069B2 (en) Neutral wire open phase detection circuit breaker
JPH022079Y2 (en)
JPH04299061A (en) Power supply
JPH03178555A (en) Inductance circuit and switching power source using the same
JPS60249874A (en) Preventing method of irregular magnetization of transformer for inverter
JPS61132086A (en) Protecting circuit of servo motor
JPH0534228Y2 (en)
JPS5828822B2 (en) switching regulator
JPH05308774A (en) Power unit
JPS61273176A (en) Inverter
JPH01202158A (en) Overcurrent detector circuit
JPH11305852A (en) Power regulation unit