JPH0219845Y2 - - Google Patents
Info
- Publication number
- JPH0219845Y2 JPH0219845Y2 JP1980132743U JP13274380U JPH0219845Y2 JP H0219845 Y2 JPH0219845 Y2 JP H0219845Y2 JP 1980132743 U JP1980132743 U JP 1980132743U JP 13274380 U JP13274380 U JP 13274380U JP H0219845 Y2 JPH0219845 Y2 JP H0219845Y2
- Authority
- JP
- Japan
- Prior art keywords
- permanent magnet
- valve body
- valve
- pressure
- magnetic pole
- 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
Links
- 239000012530 fluid Substances 0.000 claims description 17
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical group [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 claims description 15
- 230000005284 excitation Effects 0.000 claims description 5
- 238000010586 diagram Methods 0.000 description 3
- 230000003247 decreasing effect Effects 0.000 description 1
- 230000002542 deteriorative effect Effects 0.000 description 1
- 239000000696 magnetic material Substances 0.000 description 1
- 230000007704 transition Effects 0.000 description 1
- 238000011144 upstream manufacturing Methods 0.000 description 1
Landscapes
- Magnetically Actuated Valves (AREA)
- Control Of Fluid Pressure (AREA)
Description
【考案の詳細な説明】
本考案は電気信号により流体出口側の圧力を制
御できる圧力制御弁に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a pressure control valve that can control the pressure on the fluid outlet side using an electric signal.
第1図に示す従来の圧力制御弁は、流体入口1
と流体出口2との間に弁座3を有し、前記弁座3
と同軸上に弁体4が設けられ、この弁体4の上部
にダイアフラム5、ダイアフラム当板6、永久磁
石7が固着されており、前記ダイアフラム5の外
周は弁ケース8に支持されている。前記ダイアフ
ラム5と弁体4は弁体上流側、即ち1次圧室9内
における受圧面積はほぼ等しくなるよう形成され
ている。弁体下流側は2次圧室10で、流体出口
2のさらに下流に流量ノズル(図示せず)が連結
される。11はダイアフラム5により1次圧室9
と仕切られた上部空間を大気と連通するための連
通孔、12は弁ケース8に固定されたヨーク、1
3はヨーク10内の中央部に永久磁石7に対向し
て設けられた固定鉄心、14は電磁コイルであ
る。 The conventional pressure control valve shown in FIG.
a valve seat 3 between the valve seat 3 and the fluid outlet 2;
A valve body 4 is provided coaxially with the valve body 4 , and a diaphragm 5 , a diaphragm contact plate 6 , and a permanent magnet 7 are fixed to the upper part of the valve body 4 , and the outer periphery of the diaphragm 5 is supported by a valve case 8 . The diaphragm 5 and the valve body 4 are formed so that their pressure receiving areas on the upstream side of the valve body, that is, within the primary pressure chamber 9, are approximately equal. A secondary pressure chamber 10 is located downstream of the valve body, and a flow nozzle (not shown) is connected further downstream of the fluid outlet 2. 11 is a primary pressure chamber 9 formed by a diaphragm 5
12 is a yoke fixed to the valve case 8; 1 is a communication hole for communicating the upper space partitioned with the atmosphere;
Reference numeral 3 indicates a fixed iron core provided at the center of the yoke 10 facing the permanent magnet 7, and 14 indicates an electromagnetic coil.
このような従来の圧力制御弁の動作について説
明すると、流体入口1に所定の供給圧で圧送され
た流体は、1次圧室9に流入し、弁体4と弁座3
との間隙すなわち弁開度に応じて2次圧室10へ
流れ込み、流体出口2へと流れる。このときの2
次圧室10内の流体圧力つまり2次圧P2をみて
みることにする。まず弁体4に作用する力の均合
関係は、1次圧室9内の圧力つまり1次圧をP1
とし、1次圧室9側のダイアフラム受圧面積を
AD、同じく弁体受圧面積をAV、2次圧室10側
の弁体受圧面積をAVとすると次の式で表わされ
る。 To explain the operation of such a conventional pressure control valve, fluid fed under pressure to the fluid inlet 1 at a predetermined supply pressure flows into the primary pressure chamber 9, and the valve body 4 and the valve seat 3
The fluid flows into the secondary pressure chamber 10 and flows into the fluid outlet 2 according to the gap between the fluid and the valve opening degree. 2 at this time
Let's take a look at the fluid pressure in the secondary pressure chamber 10, that is, the secondary pressure P2 . First, the balance relationship of the forces acting on the valve body 4 is such that the pressure in the primary pressure chamber 9, that is, the primary pressure, is P 1
The pressure receiving area of the diaphragm on the primary pressure chamber 9 side is
Similarly, when A D is the pressure receiving area of the valve body and A V is the pressure receiving area of the valve body on the secondary pressure chamber 10 side, it is expressed by the following equation.
F+P1・AV=P1・AD+P2・AV …(1)
なおFはコイル14、固定鉄心13、ヨーク1
2、永久磁石7などによる磁気的な力Fgに弁体
4や永久磁石7の自重Wを加えた力である。 F + P 1・A V = P 1・A D +P 2・A V …(1) F is coil 14, fixed core 13, yoke 1
2. This is the force obtained by adding the weight W of the valve body 4 and the permanent magnet 7 to the magnetic force Fg caused by the permanent magnet 7, etc.
ところでP1・AVとP1・ADはほぼ等しくなるよ
う形成されているため(1)式は次のようになる。 By the way, since P 1 ·A V and P 1 ·A D are formed to be approximately equal, equation (1) becomes as follows.
F=P2・AV …(2)
したがつて2次圧P2は1次圧P1とは無関係に
永久磁石7の吸引力または電磁反発力によつて定
まり、いいかえれば電磁反発力によつて2次圧
P2が制御される。 F= P2・A V ...(2) Therefore, the secondary pressure P2 is determined by the attractive force or electromagnetic repulsion of the permanent magnet 7, regardless of the primary pressure P1.In other words, it is determined by the electromagnetic repulsion force. Therefore, secondary pressure
P 2 is controlled.
この従来の圧力制御弁の特性を第2図Aに示
す。この特性図の横軸は圧力制御弁のコイルに流
す電流Iを示し、縦軸は2次圧P2を示す。この
従来の特性で2次圧P2を0からPTの間で制御す
るためにコイル電流IはI2′からI4の間でコントロ
ールすることになる。ところがこの従来の圧力制
御弁では、永久磁石7の特性ばらつきが圧力制御
弁の特性ばらつきとなつて現われてしまう不都合
があつた。また従来の圧力制御弁においてコイル
14に電気入力を与えない場合、つまり電流が零
のとき永久磁石7と固定鉄心13との間に吸引力
が作用し、弁体4は弁座3に当接している。即ち
弁閉止状態である。2次圧P2はコイル14の電
流を次第に増大させ固定鉄心13と永久磁石7と
の間に電磁反発力が作用しはじめるコイル電流I2
から、ようやく増加しはじめる。 The characteristics of this conventional pressure control valve are shown in FIG. 2A. The horizontal axis of this characteristic diagram shows the current I flowing through the coil of the pressure control valve, and the vertical axis shows the secondary pressure P2 . With this conventional characteristic, in order to control the secondary pressure P 2 between 0 and PT , the coil current I is controlled between I 2 ' and I 4 . However, this conventional pressure control valve has the disadvantage that variations in the characteristics of the permanent magnet 7 appear as variations in the characteristics of the pressure control valve. Further, in the conventional pressure control valve, when no electrical input is applied to the coil 14, that is, when the current is zero, an attractive force acts between the permanent magnet 7 and the fixed iron core 13, and the valve body 4 comes into contact with the valve seat 3. ing. That is, the valve is in a closed state. The secondary pressure P 2 gradually increases the current in the coil 14, and the coil current I 2 causes electromagnetic repulsion to begin to act between the fixed iron core 13 and the permanent magnet 7.
It finally begins to increase.
このコイル電流I2による電磁力は固定鉄心13
と永久磁石7の間に作用している吸引力を打消す
ために必要な力であり、第2図Aに示した特性に
おいて動作開始電流I2を小さくする場合永久磁石
7の磁力を弱めることにより実現できる。しかし
それにより第2図A′に示すように制御特性のゲ
インが大きくなる。つまりコイル電流Iに対する
2次圧P2の変化量が大きくなり、若干のコイル
電流Iのばらつきにより2次圧P2が大きく変化
する結果となる。 The electromagnetic force due to this coil current I 2 is
This is the force necessary to cancel the attractive force acting between the permanent magnet 7 and the permanent magnet 7, and when reducing the operation starting current I2 with the characteristics shown in Fig. 2A, the magnetic force of the permanent magnet 7 must be weakened. This can be achieved by However, this increases the gain of the control characteristics as shown in FIG. 2A'. In other words, the amount of change in the secondary pressure P 2 with respect to the coil current I becomes large, and a slight variation in the coil current I results in a large change in the secondary pressure P 2 .
これは永久磁石7の磁力を弱めると固定鉄心1
3に対して永久磁石7が変位する際の固定鉄心1
3と永久磁石7の間に作用する磁力の変化特性が
変るためであり実用的でない。したがつて電流は
零からI2までの間は2次圧P2を制御するためには
何ら役立つておらず、いいかえれば所定の2次圧
を得るために比較的大きい電流を必要とする欠点
があつた。 When the magnetic force of the permanent magnet 7 is weakened, the fixed iron core 1
Fixed iron core 1 when permanent magnet 7 is displaced relative to 3
This is because the change characteristics of the magnetic force acting between the permanent magnet 3 and the permanent magnet 7 change, which is not practical. Therefore, the current is of no use in controlling the secondary pressure P 2 from zero to I 2 , and in other words, the disadvantage is that a relatively large current is required to obtain a predetermined secondary pressure. It was hot.
本考案は、上記従来例に鑑み、低電力で動作が
可能であり、かつ特性ばらつきの小さい圧力制御
弁を提供することを目的とするものである。 The present invention has been made in view of the above-mentioned conventional examples, and an object of the present invention is to provide a pressure control valve that can be operated with low electric power and has small variations in characteristics.
以下本考案の一実施例を図面とともに説明す
る。第3図は本考案による圧力制御弁の断面図を
示し、弁ボデイ20の流体入口21と流体出口2
2との間に弁座23を設けている。この弁座23
と同軸上に弁体24を設け、弁体24の上部には
ダイアフラム25、非磁性体からなる磁石座26
及び第1永久磁石27が装着されている。また前
記第1永久磁石27に対向して固定鉄心28の磁
極部29を設け、さらに固定鉄心28の上端部に
は、第1永久磁石27よりも弱く、かつ第1永久
磁石27と反発する方向の磁極を磁極部29に生
ずる第2永久磁石30が間隙gを形成して設けら
れている。31はヨーク、32は励磁コイル、3
3はコイルボビンであり固定鉄心28、第2永久
磁石30、ヨーク31、励磁コイル32で電磁石
が構成されている。第2永久磁石30はヨーク3
1に螺合したねじ34及び固定ナツト35からな
る調整部材36により吊り下げ固定されており、
溝37にドライバー等の工具を挿入して回動させ
ることにより固定鉄心28に対する第2永久磁石
30の相対位置を調整することができる。つまり
磁気ギヤツプとなる空隙gを自由に調整すること
が可能であり、磁極部29に発生する第2永久磁
石30の反発力を調整することができる。 An embodiment of the present invention will be described below with reference to the drawings. FIG. 3 shows a cross-sectional view of the pressure control valve according to the present invention, showing the fluid inlet 21 and fluid outlet 2 of the valve body 20.
A valve seat 23 is provided between the valve seat 2 and the valve seat 2. This valve seat 23
A valve body 24 is provided coaxially with the valve body 24, and a diaphragm 25 and a magnet seat 26 made of a non-magnetic material are provided above the valve body 24.
and a first permanent magnet 27 are attached. Further, a magnetic pole portion 29 of a fixed iron core 28 is provided opposite to the first permanent magnet 27, and a magnetic pole portion 29 of a fixed iron core 28 is provided at an upper end portion of the fixed iron core 28 in a direction that is weaker than the first permanent magnet 27 and repulsive to the first permanent magnet 27. A second permanent magnet 30 that produces a magnetic pole in the magnetic pole portion 29 is provided with a gap g formed therebetween. 31 is a yoke, 32 is an exciting coil, 3
3 is a coil bobbin, and an electromagnet is constituted by a fixed iron core 28, a second permanent magnet 30, a yoke 31, and an exciting coil 32. The second permanent magnet 30 is the yoke 3
It is suspended and fixed by an adjustment member 36 consisting of a screw 34 and a fixing nut 35 screwed into 1.
By inserting a tool such as a screwdriver into the groove 37 and rotating it, the relative position of the second permanent magnet 30 with respect to the fixed iron core 28 can be adjusted. In other words, it is possible to freely adjust the air gap g serving as a magnetic gap, and the repulsive force of the second permanent magnet 30 generated in the magnetic pole portion 29 can be adjusted.
38は電磁石ボデイでありダイアフラム25を
挾持し弁ボデイ20に固定されている。39は通
気孔、40は下蓋でありOリング41を介して洩
れなく弁ボデイ20に固定されている。 Reference numeral 38 denotes an electromagnetic body which clamps the diaphragm 25 and is fixed to the valve body 20. Reference numeral 39 is a vent hole, and 40 is a lower cover, which is fixed to the valve body 20 through an O-ring 41 without leakage.
以上の構成において励磁コイル32に通電して
いない時は第1永久磁石27と固定鉄心28は吸
引し合い、第1永久磁石27は上方に持上がる方
向に作用し、弁体24は弁座23に押しつけられ
弁は閉塞状態にある。ただしこの時、第2永久磁
石30の作用により弁体24に作用する力は、第
1永久磁石27のみの場合よりも小さい。説明上
この吸引力をFaとする。次に励磁コイル32に
通電すると前記の吸引力Faはさらに小さくなつ
て行き、コイル電流を増加して行くと前記吸引力
Faは零となり、さらにコイル電流を増加すると
Faは反発力へと移行して開弁がはじまり、弁開
度は電流に比例して増加する。この本考案の特性
図を第2図の曲線Bに示す。コイル電流I1で流体
出口22側圧力P2を制御しはじめI3で最大制御圧
PTに達する。即ち電流I1′〜I3の範囲で圧力制御が
可能である。 In the above configuration, when the excitation coil 32 is not energized, the first permanent magnet 27 and the fixed iron core 28 attract each other, the first permanent magnet 27 acts in an upward lifting direction, and the valve body 24 The valve is in a closed state. However, at this time, the force acting on the valve body 24 due to the action of the second permanent magnet 30 is smaller than when only the first permanent magnet 27 is used. For the sake of explanation, this attraction force will be referred to as Fa. Next, when the excitation coil 32 is energized, the above-mentioned attractive force Fa becomes smaller, and when the coil current is increased, the above-mentioned attractive force Fa becomes smaller.
Fa becomes zero, and when the coil current is further increased,
Fa transitions to repulsive force and the valve begins to open, and the valve opening increases in proportion to the current. A characteristic diagram of this invention is shown in curve B of FIG. The fluid outlet 22 side pressure P2 starts to be controlled with the coil current I1 , and the maximum control pressure is reached with I3 .
Reach P T. That is, pressure control is possible within the range of current I 1 ' to I 3 .
また第2永久磁石30の固定鉄心28に対する
相対位置を調整部材36により調整可能にしたた
め励磁コイル32に通電していない状態での第1
永久磁石27と磁極部29間に作用する吸引力を
調整可能であり、動作開始電流I1は0〜I3の間で
任意に設定できる。 In addition, since the relative position of the second permanent magnet 30 with respect to the fixed iron core 28 can be adjusted by the adjustment member 36, the first
The attractive force acting between the permanent magnet 27 and the magnetic pole part 29 can be adjusted, and the operation start current I1 can be arbitrarily set between 0 and I3 .
さらに従来例においては動作開始電流を小さく
する場合第1永久磁石27の磁力を弱める必要が
あるため制御特性のゲインが大きくなる不具合が
あつたが、本実施例では第2永久磁石30を設け
ることにより第1永久磁石27と磁極部29間に
作用する吸引力を低減するため、第1永久磁石3
0が変位する際の磁極部29と第1永久磁石30
の間に作用する磁力の変化率は大きく変化するこ
とがなく、制御特性のゲインを悪化させることな
く圧力制御弁の動作開始電流値を従来例よりも小
さくすることができる。 Furthermore, in the conventional example, when the operation start current is made small, it is necessary to weaken the magnetic force of the first permanent magnet 27, which causes a problem that the gain of the control characteristic becomes large, but in this example, the second permanent magnet 30 is provided. In order to reduce the attractive force acting between the first permanent magnet 27 and the magnetic pole part 29, the first permanent magnet 3
Magnetic pole part 29 and first permanent magnet 30 when 0 is displaced
The rate of change of the magnetic force acting during this period does not change significantly, and the operation start current value of the pressure control valve can be made smaller than in the conventional example without deteriorating the gain of control characteristics.
以上述べたように本考案は第2永久磁石を第1
永久磁石と固定鉄心磁極部間に作用する磁力を調
整可能に設けたことにより制御特性のゲインを大
きく変化させることなく動作開始電流値を低減で
き小さな電力で動作が可能である。 As mentioned above, the present invention replaces the second permanent magnet with the first permanent magnet.
By making the magnetic force acting between the permanent magnet and the fixed core magnetic pole part adjustable, the operation starting current value can be reduced without significantly changing the gain of the control characteristics, and operation can be performed with small electric power.
また調整部材を設けたため簡単な操作で動作開
始電流を増減でき、永久磁石の特性ばらつき、組
立誤差等による圧力制御弁の制御特性ばらつきを
大巾に減少することが可能であり、しかも必要に
応じて動作開始電流値を任意の点に設定できる圧
力制御弁を得ることができる。 In addition, since an adjustment member is provided, the operation starting current can be increased or decreased with a simple operation, and it is possible to greatly reduce variations in the control characteristics of the pressure control valve due to variations in the characteristics of the permanent magnet, assembly errors, etc. Thus, a pressure control valve whose operation start current value can be set at an arbitrary point can be obtained.
第1図は従来例を示す圧力制御弁の断面図、第
2図はコイル電流と2次圧の関係を示す特性図、
第3図は本考案の一実施例を示す圧力制御弁の断
面図である。
21……流体入口、22……流体出口、23…
…弁座、24……弁体、25……ダイアフラム、
27……第1永久磁石、28……固定鉄心、29
……磁極部、30……第2永久磁石、31……ヨ
ーク、32……励磁コイル、36……調整部材。
Fig. 1 is a sectional view of a conventional pressure control valve, Fig. 2 is a characteristic diagram showing the relationship between coil current and secondary pressure,
FIG. 3 is a sectional view of a pressure control valve showing an embodiment of the present invention. 21...Fluid inlet, 22...Fluid outlet, 23...
...valve seat, 24...valve body, 25...diaphragm,
27...First permanent magnet, 28...Fixed iron core, 29
... Magnetic pole part, 30 ... Second permanent magnet, 31 ... Yoke, 32 ... Excitation coil, 36 ... Adjustment member.
Claims (1)
弁座と同軸上に弁体を有し、この弁体に流体圧を
受けて作動するダイアフラムと第1永久磁石を装
着し、前記第1永久磁石に対向して固定鉄心磁極
部を設けるとともに、通電されると前記第1永久
磁石に対して反発する方向の磁力を発生する励磁
コイルとヨークを設け、前記固定鉄心と励磁コイ
ル及びヨークとから構成される磁気回路中に前記
第1永久磁石に対して反発する方向の磁極を前記
固定鉄心磁極部に形成する第2永久磁石と、前記
第2永久磁石と固定鉄心との相対位置を調整する
調整部材を設けた圧力制御弁。 It has a valve seat provided between a fluid inlet and a fluid outlet, a valve body coaxially with this valve seat, a diaphragm and a first permanent magnet that operate in response to fluid pressure are attached to the valve body, and a first permanent magnet is attached to the valve body. A fixed iron core magnetic pole part is provided opposite to the first permanent magnet, and an excitation coil and a yoke are provided that generate a magnetic force in a direction repulsive to the first permanent magnet when energized, and the fixed iron core, the excitation coil, and the yoke are provided. a second permanent magnet forming a magnetic pole in a direction repulsive to the first permanent magnet in the fixed core magnetic pole part in a magnetic circuit consisting of; and a relative position between the second permanent magnet and the fixed core. A pressure control valve equipped with an adjustment member for adjustment.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1980132743U JPH0219845Y2 (en) | 1980-09-17 | 1980-09-17 |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1980132743U JPH0219845Y2 (en) | 1980-09-17 | 1980-09-17 |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS5755010U JPS5755010U (en) | 1982-03-31 |
JPH0219845Y2 true JPH0219845Y2 (en) | 1990-05-31 |
Family
ID=29492975
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP1980132743U Expired JPH0219845Y2 (en) | 1980-09-17 | 1980-09-17 |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0219845Y2 (en) |
Families Citing this family (13)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0215860U (en) * | 1988-07-18 | 1990-01-31 | ||
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JP5952150B2 (en) * | 2012-09-27 | 2016-07-13 | 株式会社ケーヒン | Solenoid valve for fuel cell |
US9201036B2 (en) | 2012-12-21 | 2015-12-01 | Fresenius Medical Care Holdings, Inc. | Method and system of monitoring electrolyte levels and composition using capacitance or induction |
US9157786B2 (en) | 2012-12-24 | 2015-10-13 | Fresenius Medical Care Holdings, Inc. | Load suspension and weighing system for a dialysis machine reservoir |
US9354640B2 (en) | 2013-11-11 | 2016-05-31 | Fresenius Medical Care Holdings, Inc. | Smart actuator for valve |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5166528A (en) * | 1974-12-06 | 1976-06-09 | Matsushita Electric Ind Co Ltd | MIZUSEIGYOKI |
Family Cites Families (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS599283Y2 (en) * | 1978-04-03 | 1984-03-23 | 三菱電機株式会社 | control valve |
-
1980
- 1980-09-17 JP JP1980132743U patent/JPH0219845Y2/ja not_active Expired
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5166528A (en) * | 1974-12-06 | 1976-06-09 | Matsushita Electric Ind Co Ltd | MIZUSEIGYOKI |
Also Published As
Publication number | Publication date |
---|---|
JPS5755010U (en) | 1982-03-31 |
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