JPH022028B2 - - Google Patents
Info
- Publication number
- JPH022028B2 JPH022028B2 JP58212722A JP21272283A JPH022028B2 JP H022028 B2 JPH022028 B2 JP H022028B2 JP 58212722 A JP58212722 A JP 58212722A JP 21272283 A JP21272283 A JP 21272283A JP H022028 B2 JPH022028 B2 JP H022028B2
- Authority
- JP
- Japan
- Prior art keywords
- current
- valve
- electromagnetic proportional
- proportional valve
- transistor amplifier
- 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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Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F7/00—Magnets
- H01F7/06—Electromagnets; Actuators including electromagnets
- H01F7/08—Electromagnets; Actuators including electromagnets with armatures
- H01F7/18—Circuit arrangements for obtaining desired operating characteristics, e.g. for slow operation, for sequential energisation of windings, for high-speed energisation of windings
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- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Magnetically Actuated Valves (AREA)
Description
【発明の詳細な説明】
産業上の利用分野
本発明は電流に応じて流体流量を制御する電磁
比例弁制御装置に関し、特に小さく良好なヒステ
リシスでかつ安定した流量特性となるように作動
させることが可能な制御装置の構成に関する。DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to an electromagnetic proportional valve control device that controls fluid flow rate according to current, and in particular can be operated to have small and good hysteresis and stable flow characteristics. Concerning possible control device configurations.
従来例の構成とその問題点
電磁比例弁はガス湯沸器やガス暖房器・ガス調
理器などにおいて、制御すべき温度負荷に対応し
てバーナへのガス供給量を制御するものである
が、電磁プランジヤ摺動式の前記弁にあつては、
弁体の動き始めは静摩擦力に打ち勝つ力が発生す
るまで動かず、弁体が止まる時は動摩擦力と駆動
力が一致した時点で止まつてしまい、摩擦力に見
合うだけの誤差や、プランジヤやヨークの残留磁
気によるヒステリシスなどで、比例弁コイルの電
流に対し、正確で再現性の高い流量制御ができな
い。そこで従来ヒステリシス特性等を良好ならし
めるために、次のような制御装置が公知である。Conventional structure and its problems Electromagnetic proportional valves are used in gas water heaters, gas heaters, gas cookers, etc. to control the amount of gas supplied to the burner in response to the temperature load to be controlled. In the case of the electromagnetic plunger sliding type valve,
When the valve body starts to move, it does not move until a force is generated that overcomes the static friction force, and when the valve body stops, it stops when the dynamic friction force and the driving force match, and there is an error that is commensurate with the friction force, and the plunger and yoke Due to hysteresis caused by residual magnetism, accurate and highly reproducible flow rate control of the proportional valve coil current cannot be performed. Conventionally, the following control device is known in order to improve the hysteresis characteristics and the like.
この場合の制御回路は第1図に示されるが、交
流電源1を整流器2によつて全波整流し、電磁比
例弁のコイル3とトランジスタ増幅器4および抵
抗5からなる直列回路に脈流の直流電流を流通さ
せて、プランジヤを微振動させながら所定の制御
をするようにしたものである。 The control circuit in this case is shown in Fig. 1, in which the AC power source 1 is full-wave rectified by a rectifier 2, and a pulsating DC current is passed through a series circuit consisting of a coil 3 of an electromagnetic proportional valve, a transistor amplifier 4, and a resistor 5. A current is passed through the plunger to cause the plunger to vibrate in a predetermined manner.
そして比例弁コイル3に流す電流の平均値を変
えるためには、第2図に示すように、全波整流の
直流をそのまま加える最大電流値(第2図イ参
照)から設定レベル以上の波高部分をカツトして
得られる所望値(第2図ロ,ハ参照)の範囲内で
電流制御を行わせており、この制御を電流調整回
路6によつて無段階的に成している。 In order to change the average value of the current flowing through the proportional valve coil 3, as shown in Figure 2, the wave height part above the set level is calculated from the maximum current value (see Figure 2 A) where full-wave rectified direct current is applied as is. The current is controlled within the range of the desired value obtained by cutting the current (see FIG. 2 B and C), and this control is performed steplessly by the current adjustment circuit 6.
この他に、サイリスタ利用による位相制御方式
によつて電流制御する形態のものもある。 In addition, there is also a type in which current is controlled by a phase control method using a thyristor.
ところが上記従来方式によつたのでは、デイザ
(出力電流波形)効果が弱くなつて初期の目的を
達成し難い問題があり、この欠点は特に低電流域
において顕著に現れるため、電磁比例弁の性能が
十分に発揮されなかつた。 However, with the above conventional method, there is a problem that the dither (output current waveform) effect becomes weak and it is difficult to achieve the initial purpose.This drawback is especially noticeable in the low current range, so the performance of the electromagnetic proportional valve is affected. I wasn't able to perform to my full potential.
上記欠点を補なうべく他の従来例として次のよ
うな制御装置が公知である。 In order to compensate for the above drawbacks, the following control device is known as another conventional example.
この場合の制御回路は第3図に示すように、直
流電源7にトランジスタ増幅器4と電磁比例弁の
コイル3を直列接続し、トランジスタ増幅器4の
ベース端子に方形波信号発生回路8を接続した構
成で、方形波信号発生回路8は第4図ニ,ホ,ヘ
のように方形波の波高値(振幅)および周期は一
定で、オンとオフとの時間比(デユーテイ)を変
化させて、平均電圧値の異なる出力信号を出さ
せるものである。なお電磁比例弁3と並列に抵抗
5とダイオード9とを直列にして接続しているの
は、弁コイル3のサージ電圧を吸収するためであ
る。 As shown in FIG. 3, the control circuit in this case has a configuration in which a transistor amplifier 4 and a coil 3 of an electromagnetic proportional valve are connected in series to a DC power supply 7, and a square wave signal generating circuit 8 is connected to the base terminal of the transistor amplifier 4. The square wave signal generating circuit 8, as shown in FIG. It outputs output signals with different voltage values. The reason why a resistor 5 and a diode 9 are connected in series in parallel with the electromagnetic proportional valve 3 is to absorb the surge voltage of the valve coil 3.
上記の従来例においては、電磁比例弁のコイル
3に断続方形波電圧が印加され、弁コイル3の電
圧および電流波形が第5図のように急な立上り・
立下りとなるために、電磁比例弁のプランジヤお
よび弁体の不規則な振動を誘発し、第6図のよう
に正常な流量特性トからずれ、チのような乱れた
流量特性になつたりする、いわゆる特性乱れを発
生しやすい問題があつた。この従来方式のように
一定周期と一定振幅の条件において、立上り・立
下りが緩やかになるようにしようとすると、周期
を長くしなければならず、そうすると最初の従来
例と同様に十分なデイザ効果が得られなくなつて
しまう。また商用電源を整流し完全平滑しないで
脈流成分を残した直流電圧を、電磁比例弁のコイ
ル3とトランジスタ増幅器4の直列回路に印加
し、脈流成分をデイザ効果として利用しようとす
る方式も公知であるが、脈流周波数が50Hzもしく
は60Hzに限定され、やはり十分なデイザ効果を得
ることができなかつた。 In the above conventional example, an intermittent square wave voltage is applied to the coil 3 of the electromagnetic proportional valve, and the voltage and current waveforms of the valve coil 3 have a sudden rise and rise as shown in FIG.
This causes irregular vibrations in the plunger and valve body of the electromagnetic proportional valve, causing the flow rate to deviate from the normal flow rate as shown in Figure 6, and become turbulent as shown in Figure 6. However, there was a problem in that so-called characteristic disturbances were likely to occur. If you try to make the rise and fall gradual under the conditions of constant period and constant amplitude as in this conventional method, the period must be made longer, and then, as in the first conventional example, a sufficient dither effect cannot be achieved. It becomes impossible to obtain it. There is also a method in which the commercial power source is rectified and a DC voltage that is not completely smoothed, leaving a pulsating component, is applied to the series circuit of the electromagnetic proportional valve's coil 3 and the transistor amplifier 4, and the pulsating component is used as a dither effect. Although this is known, the frequency of the pulsating flow is limited to 50 Hz or 60 Hz, and a sufficient dither effect cannot be obtained.
発明の目的
本発明はかかる従来の問題を解消するもので、
十分なデイザ効果を得ることができ、かつ不規則
な弁振動を起こしにくい、良好なヒステリシスで
安定した流量特性になるよう作動させる電磁比例
弁制御装置を得ることを目的とする。Purpose of the invention The present invention solves such conventional problems,
It is an object of the present invention to provide an electromagnetic proportional valve control device that can obtain a sufficient dither effect, is less likely to cause irregular valve vibrations, and operates so as to have stable flow characteristics with good hysteresis.
発明の構成
この目的を達成するために本発明は、直流電源
に弁コイルとトランジスタ増幅器を直列接続し、
直流電圧レベルを可変する電流制御回路と、前記
電流制御回路の出力が低電流時から高電流時まで
一定の周期・振幅の電圧波形を発生するデイザ発
生回路と、前記デイザ発生回路と電流制御回路と
の信号を加算する加算回路とを有し、前記加算回
路の出力信号を前記トランジスタ増幅器のベース
端子に接続するとともに、前記トランジスタ増幅
器のコレクタ−エミツタ方向と並列にコンデンサ
を接続したものである。この構成によつて電磁比
例弁コイルに流れる平均電流レベルを変化させた
場合において、弁コイルの電流はデイザ効果上、
最も好ましい一定周期・振幅でかつ緩やかな立上
り・立下りの電流波形となるよう作用する。Structure of the Invention In order to achieve this object, the present invention connects a valve coil and a transistor amplifier in series to a DC power supply,
a current control circuit that varies a DC voltage level; a dither generation circuit that generates a voltage waveform with a constant period and amplitude from a low current to a high current output from the current control circuit; and the dither generation circuit and the current control circuit. The output signal of the adder circuit is connected to the base terminal of the transistor amplifier, and a capacitor is connected in parallel with the collector-emitter direction of the transistor amplifier. With this configuration, when the average current level flowing through the electromagnetic proportional valve coil is changed, the current in the valve coil changes due to the dither effect.
It acts to provide a current waveform with the most preferable constant period and amplitude and gradual rise and fall.
実施例の説明
以下本発明の一実施例を第7図を用いて説明す
る。第7図において直流電源10に電磁比例弁の
コイル11とトランジスタ増幅器12と抵抗13
を直列接続し、弁コイル11と並列にダイオード
14を、トランジスタ12と並列にコンデンサ1
5をそれぞれ接続し、さらにデイザ発生回路16
と電流制御回路17の出力を加算回路18に入力
するように接続し、かつ加算回路18の出力端子
をトランジスタ12のベース端子に接続されてい
る。DESCRIPTION OF EMBODIMENTS An embodiment of the present invention will be described below with reference to FIG. In FIG. 7, a DC power supply 10 includes a coil 11 of an electromagnetic proportional valve, a transistor amplifier 12, and a resistor 13.
are connected in series, a diode 14 is connected in parallel with the valve coil 11, and a capacitor 1 is connected in parallel with the transistor 12.
5 are connected to each other, and a dither generating circuit 16 is connected to the
and the output of the current control circuit 17 are connected to be input to an adder circuit 18, and the output terminal of the adder circuit 18 is connected to the base terminal of the transistor 12.
上記構成においてデイザ発生回路16で発生す
る電圧波形は、電磁比例弁にとつてヒステリシス
を小さくでき、かつ不都合な弁振動を生じない最
適な一定周期一定振幅に設定し、該デイザ発生回
路16の信号と電流制御回路17の直流電圧信号
が加算回路18で加算され、トランジスタ12の
ベース電流波形は第8図のように大きい平均電流
IBHのときと、小さい平均電流IBLのときと周期・
振幅は変化せず一定となるよう作用する。このと
き、電磁比例弁のコイル11の電流波形は第9図
のように略台形波形になるように作用する。理由
を説明すると、まずトランジスタ12のベース電
流が急に立下がると、トランジスタ12のコレク
タ−エミツタ間の電気抵抗が急に増大したのと同
様に考えることができ、トランジスタ12のコレ
クタ電流は急に減少する。ところがトランジスタ
12と並列にコンデンサ15が接続してあるた
め、コンデンサ15に充電され弁コイル11には
この充電電流が流れる。このときコンデンサ15
に充電されていくにしたがつて次第に充電電流は
減少していく。以上のことからベース電流が急に
立下がつた際、弁コイル11の電流は緩やかに減
少していくことになる。逆にベース電流が立上が
る場合、コンデンサ15に充電された電荷がトラ
ンジスタ12を経て放電されるため、弁コイル1
1の電流はコンデンサ放電電流の減少につれて増
加することになり、緩やかに増大することにな
る。したがつて電磁比例弁のコイル11の電流
は、第9図のように略台形波形で変化するように
作用し、緩やかな立上り立下がりの電流変化のた
め不都合な弁振動がなく、優れたデイザ効果でヒ
ステリシスの小さい安定した比例流量特性を得ら
れる効果がある。 In the above configuration, the voltage waveform generated by the dither generating circuit 16 is set to an optimal constant period constant amplitude that can reduce hysteresis for the electromagnetic proportional valve and does not cause undesirable valve vibration, and the voltage waveform of the dither generating circuit 16 is and the DC voltage signal of the current control circuit 17 are added in the adder circuit 18, and the base current waveform of the transistor 12 becomes a large average current as shown in FIG.
When I BH , when the average current I BL is small, and when the period
It acts so that the amplitude does not change and remains constant. At this time, the current waveform of the coil 11 of the electromagnetic proportional valve acts in a substantially trapezoidal waveform as shown in FIG. To explain the reason, first, when the base current of transistor 12 suddenly falls, it can be thought of as if the electric resistance between the collector and emitter of transistor 12 suddenly increased, and the collector current of transistor 12 suddenly decreased. Decrease. However, since the capacitor 15 is connected in parallel with the transistor 12, the capacitor 15 is charged and this charging current flows through the valve coil 11. At this time, capacitor 15
The charging current gradually decreases as the battery is charged. From the above, when the base current suddenly falls, the current in the valve coil 11 will gradually decrease. Conversely, when the base current rises, the charge stored in the capacitor 15 is discharged via the transistor 12, so that the valve coil 1
The current of 1 will increase as the capacitor discharge current decreases, and will increase gradually. Therefore, the current in the coil 11 of the electromagnetic proportional valve changes in a substantially trapezoidal waveform as shown in FIG. The effect is that stable proportional flow characteristics with small hysteresis can be obtained.
発明の効果
以上のように本発明の電磁比例弁制御装置によ
れば次の効果が得られる。Effects of the Invention As described above, the electromagnetic proportional valve control device of the present invention provides the following effects.
(1) 一定周期・振幅の波形を発生するデイザ発生
回路と電流制御回路との信号を加算回路で加算
し、トランジスタベース端子に入力し、かつト
ランジスタと並列にコンデンサを接続した構成
としているので、弁コイルの電流は緩やかな立
上り立下がりの略台形波形となるよう作用し、
有効なデイザ効果を発揮しながら不都合な弁振
動を誘起しないため、小さく良好なヒステリシ
スでかつ安定した流量特性となるよう電磁比例
弁を作動させることができる効果がある。(1) The signals from the dither generation circuit that generates a waveform with a constant period and amplitude and the current control circuit are added by an adder circuit, and the result is input to the transistor base terminal, and a capacitor is connected in parallel with the transistor. The current in the valve coil acts in a roughly trapezoidal waveform with gradual rises and falls.
Since no undesirable valve vibration is induced while exhibiting an effective dither effect, the electromagnetic proportional valve can be operated with small and good hysteresis and stable flow characteristics.
(2) デイザ発生回路によるデイザ信号と、電流制
御回路による直流信号とを加算し、弁コイルと
直列接続のトランジスタベース端子に入力する
構成であるから、デイザ波形および周期・振幅
を任意かつ最適なものに設定ができ、各種の電
磁比例弁に対応できる。電磁比例弁の可動部・
弁体などの形態や重量などにより、最もデイザ
効果を発揮できる波形および周期・振幅はそれ
ぞれ条件が異なる場合が多い、また不都合な弁
振動を生じる条件についても同様であり、上記
の本発明の構成によれば、それらを最適な条件
で作動させることが可能となるわけである。(2) Since the dither signal from the dither generation circuit and the DC signal from the current control circuit are added together and input to the transistor base terminal connected in series with the valve coil, the dither waveform, period, and amplitude can be set arbitrarily and optimally. It can be set to various types of solenoid proportional valves. Moving parts of electromagnetic proportional valves
Depending on the shape and weight of the valve body, etc., the conditions for the waveform, period, and amplitude that can best exhibit the dither effect are often different, and the same is true for the conditions that cause undesirable valve vibration. According to this, it is possible to operate them under optimal conditions.
(3) 低電流時から高電流時まで、常に一定の周期
振幅のデイザ波形で作動する方式であるため、
電磁比例弁の作動位置および流量位置がどこに
あつても、常に最適な一定のデイザ効果が得ら
れ、常に安定した特性を得ることができる。(3) Since the method operates with a dither waveform with a constant periodic amplitude from low current to high current,
No matter where the operating position and flow rate position of the electromagnetic proportional valve are, a certain optimum dither effect can always be obtained, and stable characteristics can always be obtained.
第1図は従来の電磁比例弁制御装置の一例を示
す基本回路図、第2図イ〜ハは第1図に示す装置
による弁コイルの電流波形線図、第3図は他の従
来の電磁比例弁制御装置の一例を示す基本回路
図、第4図ニ〜ヘは第3図に示す装置の方形波発
生回路の出力波形線図、第5図は第3図に示す装
置の弁コイルの電圧・電流波形線図、第6図は第
3図に示す装置による電磁比例弁流量特性図、第
7図は本発明の電磁比例弁制御装置の一実施例を
示す基本回路図、第8図は第7図に示す装置のト
ランジスタベース電流波形線図、第9図は第7図
に示す装置の弁コイル電流波形線図である。
10……直流電源、11……弁コイル、12…
…トランジスタ増幅器、15……コンデンサ、1
6……デイザ発生回路、17……電流制御回路、
18……加算回路。
Fig. 1 is a basic circuit diagram showing an example of a conventional electromagnetic proportional valve control device, Fig. 2 A to C are current waveform diagrams of the valve coil by the device shown in Fig. 1, and Fig. 3 is a basic circuit diagram showing an example of a conventional electromagnetic proportional valve control device. A basic circuit diagram showing an example of a proportional valve control device, Figures 4(d) to 4(f) are output waveform diagrams of the square wave generation circuit of the device shown in FIG. 3, and FIG. 5 is a diagram of the valve coil of the device shown in FIG. Voltage/current waveform diagram, Fig. 6 is a flow rate characteristic diagram of the electromagnetic proportional valve according to the device shown in Fig. 3, Fig. 7 is a basic circuit diagram showing an embodiment of the electromagnetic proportional valve control device of the present invention, Fig. 8 is a transistor base current waveform diagram of the device shown in FIG. 7, and FIG. 9 is a valve coil current waveform diagram of the device shown in FIG. 10...DC power supply, 11...Valve coil, 12...
...Transistor amplifier, 15...Capacitor, 1
6... dither generation circuit, 17... current control circuit,
18...Addition circuit.
Claims (1)
直列接続し、直流電圧レベルを可変する電流制御
回路と、前記電流制御回路の出力が低電流時から
高電流時まで一定の周期・振幅の電圧波形を発生
するデイザ発生回路と、前記デイザ発生回路と電
流制御回路との信号を加算する加算回路とを有
し、前記加算回路の出力信号を前記トランジスタ
増幅器のベース端子に接続するとともに、前記ト
ランジスタ増幅器のコレクタ−エミツタ方向と並
列にコンデンサを接続してなる電磁比例弁制御装
置。1. A valve coil and a transistor amplifier are connected in series to a DC power supply, and a current control circuit that varies the DC voltage level, and the output of the current control circuit generates a voltage waveform with a constant period and amplitude from low current to high current. and an adder circuit that adds signals from the dither generator and current control circuit, the output signal of the adder being connected to the base terminal of the transistor amplifier, and the collector of the transistor amplifier being connected to the base terminal of the transistor amplifier. - An electromagnetic proportional valve control device consisting of a capacitor connected in parallel with the emitter direction.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58212722A JPS60104874A (en) | 1983-11-11 | 1983-11-11 | Control device of proportional solenoid valve |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58212722A JPS60104874A (en) | 1983-11-11 | 1983-11-11 | Control device of proportional solenoid valve |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60104874A JPS60104874A (en) | 1985-06-10 |
| JPH022028B2 true JPH022028B2 (en) | 1990-01-16 |
Family
ID=16627346
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58212722A Granted JPS60104874A (en) | 1983-11-11 | 1983-11-11 | Control device of proportional solenoid valve |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60104874A (en) |
Family Cites Families (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6116770Y2 (en) * | 1977-06-09 | 1986-05-23 | ||
| JPS5854283A (en) * | 1981-09-26 | 1983-03-31 | Omron Tateisi Electronics Co | Driving circuit for proportional valve |
-
1983
- 1983-11-11 JP JP58212722A patent/JPS60104874A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS60104874A (en) | 1985-06-10 |
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