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JPS6134029B2 - - Google Patents
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JPS6134029B2 - - Google Patents

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Publication number
JPS6134029B2
JPS6134029B2 JP13807578A JP13807578A JPS6134029B2 JP S6134029 B2 JPS6134029 B2 JP S6134029B2 JP 13807578 A JP13807578 A JP 13807578A JP 13807578 A JP13807578 A JP 13807578A JP S6134029 B2 JPS6134029 B2 JP S6134029B2
Authority
JP
Japan
Prior art keywords
amount
electromagnet
energization
secondary pressure
control valve
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
Application number
JP13807578A
Other languages
Japanese (ja)
Other versions
JPS5563074A (en
Inventor
Michio Fujiwara
Eiji Nozawa
Motohiro Takahashi
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi 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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP13807578A priority Critical patent/JPS5563074A/en
Publication of JPS5563074A publication Critical patent/JPS5563074A/en
Publication of JPS6134029B2 publication Critical patent/JPS6134029B2/ja
Granted legal-status Critical Current

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  • Magnetically Actuated Valves (AREA)

Description

【発明の詳細な説明】 本発明は電磁石の励磁コイルに電流を通電する
ことによりこの電流の通電量に応じて2次圧(吐
出圧)を制御する流量制御弁に関し、特に、2次
圧の制御幅を拡大するための制御装置に関するも
のである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a flow control valve that controls secondary pressure (discharge pressure) according to the amount of current passed through an excitation coil of an electromagnet. The present invention relates to a control device for expanding control width.

第1図は流量制御弁の構成を示す図で、この流
量制御弁は制御弁部1と電磁石部5とで成り、制
御弁部1には、1次室1aに流体を供給する1次
口1bを、2次室1cから流体を吐出する2次口
1dを備えるとともに弁座2と、弁体3及びダイ
ヤフラム4とを備えている。また、電磁石部5に
はヨーク6と、中心磁極7とを備えてこのヨーク
6と中心磁極7間の開磁路部を円環状に構成し、
周方向の均一な磁界を形成し、かつ、永久磁石8
と励磁コイル9を備えて励磁コイル9に所定方向
の電流を通電することにより中心磁極7と永久磁
石8との対向面側を同極性として周方向の均一な
磁気反発力を得られるようにしている。そして、
この磁石反発力は均圧板10を介して制御弁部1
のダイヤフラム4に外力Fとして作用するように
している。
FIG. 1 is a diagram showing the configuration of a flow control valve. This flow control valve consists of a control valve part 1 and an electromagnet part 5. The control valve part 1 has a primary port for supplying fluid to a primary chamber 1a. 1b is provided with a secondary port 1d for discharging fluid from the secondary chamber 1c, and also includes a valve seat 2, a valve body 3, and a diaphragm 4. Further, the electromagnet section 5 is provided with a yoke 6 and a center magnetic pole 7, and an open magnetic path section between the yoke 6 and the center magnetic pole 7 is configured in an annular shape.
A permanent magnet 8 forms a uniform magnetic field in the circumferential direction.
and an excitation coil 9, and by supplying current in a predetermined direction to the excitation coil 9, the facing sides of the central magnetic pole 7 and the permanent magnet 8 are made to have the same polarity, and a uniform magnetic repulsion force in the circumferential direction can be obtained. There is. and,
This magnetic repulsion force is applied to the control valve section 1 via the pressure equalizing plate 10.
The external force F acts on the diaphragm 4.

上記により構成される流量制御弁において、供
給源から圧送された流体は1次口1bから入りダ
イヤフラム4に作用する外力Fにより弁座2と弁
体3との間隙即ち、弁開度に応じてその流量が制
限され2次口1dを経て図示しない流量ノズルに
吐出される。この際、制御弁部1の1次室1aで
の1次圧をP1とし、2次室1cでの2次圧をP2
すれば、 F=P1AD+P2AV−P1AV ……(1) ここで ADはダイヤフラム4の受圧面積 AVは弁体3の受圧面積 なる関係式が得られ、さらに、AD〓AVとなる様
に設計すれば、式(1)は F〓P2AV ……(2) となる。即ち、流量制御弁の2次圧P2は1次圧P1
の変動に拘らずダイヤフラム4に作用する外力F
つまり、電磁石部5での磁気的反発力により決定
することができる。
In the flow rate control valve configured as described above, the fluid pumped from the supply source enters through the primary port 1b and is controlled by the external force F acting on the diaphragm 4 depending on the gap between the valve seat 2 and the valve body 3, that is, depending on the valve opening degree. Its flow rate is restricted and it is discharged through a secondary port 1d to a flow nozzle (not shown). At this time, if the primary pressure in the primary chamber 1a of the control valve part 1 is P 1 and the secondary pressure in the secondary chamber 1c is P 2 , then F=P 1 A D +P 2 A V −P 1 A V ...(1) Here, A D is the pressure receiving area of the diaphragm 4, A V is the pressure receiving area of the valve body 3, and if the design is made so that A D = A V , then the formula (1) becomes F〓P 2 A V ……(2). In other words, the secondary pressure P 2 of the flow control valve is the primary pressure P 1
The external force F acting on the diaphragm 4 regardless of the fluctuation of
In other words, it can be determined by the magnetic repulsion force in the electromagnet section 5.

ところで、この流量制御弁により燃焼装置(図
示せず)への燃料流量の制御を行なうことによつ
て燃焼装置内の室温又は湯温等の温度制御をする
場合には、流量制御弁は燃焼装置の特性に応じて
所定値以上の2次圧すなわち下限2次圧以上の圧
力を得なくてはならず、下限2次圧以下の燃焼量
で燃焼させる時には燃焼装置のバーナーに逆火を
引き起こし、不完全燃焼に到ることになる。故
に、流量制御弁の電磁石部5の励磁コイル9への
通電量を、下限2次圧を与える最小通電量以上と
上限2次圧を与える最大通電量以下との範囲にお
いて可変させ、これにより所定の温度となるよう
に2次圧を制御することを要する。
By the way, when controlling the temperature such as the room temperature or hot water temperature in the combustion device by controlling the fuel flow rate to the combustion device (not shown) using this flow control valve, the flow control valve is not connected to the combustion device. It is necessary to obtain a secondary pressure above a predetermined value, that is, a pressure above the lower limit secondary pressure according to the characteristics of This will lead to incomplete combustion. Therefore, the amount of current applied to the excitation coil 9 of the electromagnet portion 5 of the flow control valve is varied within the range of more than the minimum amount of current that provides the lower limit secondary pressure and less than or equal to the maximum amount of current that provides the upper limit secondary pressure. It is necessary to control the secondary pressure so that the temperature becomes .

しかるに、流量制御弁の通電量Iに対する2次
圧P2の特性は、第2図で明らかのように、下限2
次圧P2Lを得る最小電量ILから通電量を増加し
て通電量IMで上限2次圧P2Mを得たのち、通電
量を減少させて最小通電量ILまで減じても2次
圧は下限2次圧P2Lを得られず。P2L′の値までし
か下げることができない。これは電磁石部5を構
成するヨーク6、中心磁極7等の磁路における磁
気ヒステリシスの特性に起因するもので、通電量
の増加時と減少時とでは2次圧は、異なる軌跡を
たぞつてヒステリシスループを描き、2次圧が零
となる通電量においては、電磁石の保磁力に相当
するΔIの通電量の差が生じる。したがつて、通
電量増加時に下限2次圧を得る最小通電量IL
通電量減少時に適用する場合には保持力により実
質上2次圧の制御幅が非常に小さいものになると
いう欠点を有していた。一方、下限2次圧P2Lを
最小通電量IL′で得られる様に構成した場合に
は、通電量をI0の時点において減少させたときに
は、第2図中一点鎖線で示すように上記最大通電
量をIMとする減少時の軌跡とは異なる軌跡をた
どつて最小通電量IL′では下限2次圧P2L″を得
ることになり、この下限2次圧P2L″は下限2次
圧P2Lよりも小さい値を示すため燃焼装置のバー
ナーに逆火を引き起すことになる。したがつて、
実質的に通電量はILの時点までしか減少させる
ことができず2次圧の制御幅が小さいものになつ
ていた。
However, as is clear from Fig. 2, the characteristics of the secondary pressure P2 with respect to the amount of current I of the flow control valve are lower limit 2.
Even if the energization amount is increased from the minimum energization amount I L to obtain the next pressure P 2 L to obtain the upper limit secondary pressure P 2 M with the energization amount I M , and then the energization amount is decreased to the minimum energization amount I L. The lower limit secondary pressure P 2 L could not be obtained for the secondary pressure. It can only be reduced to the value of P 2 L′. This is due to the characteristics of magnetic hysteresis in the magnetic path of the yoke 6, center magnetic pole 7, etc. that make up the electromagnet section 5, and the secondary pressure follows different trajectories when the amount of energization increases and when it decreases. At the amount of current at which a hysteresis loop is drawn and the secondary pressure is zero, a difference in the amount of current of ΔI corresponding to the coercive force of the electromagnet occurs. Therefore, when applying the minimum energization amount I L to obtain the lower limit secondary pressure when the energization amount increases, when the energization amount is decreased, there is a drawback that the control width of the secondary pressure becomes very small due to the holding force. had. On the other hand, if the configuration is such that the lower limit secondary pressure P 2 L can be obtained with the minimum amount of energization I L ′, when the amount of energization is decreased at the time of I 0 , as shown by the dashed line in FIG. The lower limit secondary pressure P 2 L'' is obtained at the minimum energization amount I L ′ by following a different trajectory from the trajectory when decreasing when the maximum energization amount is I M , and this lower limit secondary pressure P 2 L '' indicates a value smaller than the lower limit secondary pressure P 2 L, which will cause backfire in the burner of the combustion device. Therefore,
Substantially, the amount of energization can only be reduced up to the point of I L , resulting in a narrow control range of the secondary pressure.

本発明は上記のような従来のものの欠点に鑑み
てなされたもので、流量制御弁の電磁石部への通
電開始時から最大通電量で電磁石の磁路が完全に
磁化されるまでは、電磁石が制御信号により通電
量を増減制御されるのを禁止し、電磁石へ上限2
次圧を与える所定の時限信号を発生する時限信号
発生器を設け、この最大通電量に応じた電磁石の
保持力により通電量を増減しても最小通電量にお
ける下限2次圧が常に一定値を得ることができる
マイナーループを確立し、2次圧の制御幅を拡大
することができる制御装置を提供することを目的
としている。
The present invention was made in view of the above-mentioned drawbacks of the conventional ones, and the electromagnet is not activated until the magnetic path of the electromagnet is completely magnetized with the maximum amount of current applied from the time when the electromagnetic part of the flow control valve starts being energized. Prohibits the amount of energization from being increased or decreased by control signals, and sets the upper limit of 2 to the electromagnet.
A time signal generator is provided to generate a predetermined time signal to give the next pressure, and the lower limit secondary pressure at the minimum amount of energization is always kept at a constant value even if the amount of energization is increased or decreased by the holding force of the electromagnet according to the maximum amount of energization. It is an object of the present invention to provide a control device that can establish a minor loop that can be obtained and expand the control range of secondary pressure.

以下、本発明の一実施例を図について説明す
る。第3図において、11は第1図に示す構造の
流量制御弁、12は流量制御弁11から所定2次
圧の燃料流量を受けて燃焼装置のバーナーの燃焼
により加熱された温風又は、温湯を得る燃焼装置
の熱交換部、13は上記温風又は、温湯の温度を
検出して、この温度に応じた信号を出力する温度
検出装置、14は設定温度と上記温度検出装置1
3の検出温度との温度差に応じて電磁石への通電
量を制御する信号を出力するとともに最大通電量
と最小通電量とを決定することができる機能を有
した演算増幅器、15は流量制御弁11の電磁石
部5への通電開始時に演算増幅器14を介して所
定の上限2次圧を与える最大通電量の電流を設定
時間出力するように動作させる時限信号発生器で
ある。
Hereinafter, one embodiment of the present invention will be described with reference to the drawings. In FIG. 3, reference numeral 11 indicates a flow rate control valve having the structure shown in FIG. 13 is a temperature detection device that detects the temperature of the hot air or hot water and outputs a signal according to this temperature; 14 is a set temperature and the temperature detection device 1;
15 is a flow rate control valve; 15 is an operational amplifier having a function of outputting a signal for controlling the amount of current applied to the electromagnet according to the temperature difference between the detected temperature of 3 and determining the maximum amount of current and the minimum amount of current applied; This is a time signal generator that operates so as to output a maximum amount of current for a set time to provide a predetermined upper limit secondary pressure via an operational amplifier 14 when the electromagnet section 11 starts being energized.

したがつて、上記構成による流量制御弁の制御
装置は先ず、流量制御弁11の電磁石部5への通
電開始に際して、時限信号発生器15が所定時間
動作してこれにより演算増幅器14は流量制御弁
11の電磁石部5に最大通電量IMが通電される
よう制御信号を出力する。最大通電量IMが通電
されて上限2次圧P2Mを得た流量制御弁11には
その後、燃焼装置の熱交換部12の検出温度と設
定温度との温度差に応じた通電量の電流が通電さ
れて2次圧が制御される。このとき、この流量制
御弁の制御装置では上記2次圧P2Mと燃焼装置の
バーナーの特性に応じて定まる下限2次圧P2Lと
の制御幅内で流量制御弁11の2次圧が制御され
る。即ち、第4図に示される動作特性図で、流量
制御弁11が動作開始時には2次圧はA点にあ
り、その後、すなわち上記時限信号発生器15の
動作時間が終了した後は、点Aから通電量を減少
させると点Bに至り、最小通電量ILで所定の2
次圧PBが得られる。次にこの点Bから今度は通
電量を増大させると点Cに至る。さらにこの点に
おける通電量から通電量を減少させて最小通電量
Lに設定すると点Dに至り、上記2次圧PBより
低い所定の2次圧が得られる。点Dからさらに通
電量を増大させて行くときのマイナーループは点
C′で主ループ(X―A)に交差する。
Therefore, in the flow control valve control device having the above configuration, first, when starting energization to the electromagnet section 5 of the flow control valve 11, the time signal generator 15 operates for a predetermined period of time, thereby causing the operational amplifier 14 to control the flow control valve. A control signal is outputted so that the maximum amount of current I M is applied to the electromagnet portion 5 of No. 11. The flow rate control valve 11, which has been energized with the maximum amount of current I M and obtained the upper limit secondary pressure P 2 M, is then energized with the amount of current that corresponds to the temperature difference between the detected temperature of the heat exchange section 12 of the combustion device and the set temperature. Current is applied to control the secondary pressure. At this time, the flow control valve control device controls the secondary pressure of the flow control valve 11 within a control range between the secondary pressure P 2 M and the lower limit secondary pressure P 2 L determined according to the characteristics of the burner of the combustion device. is controlled. That is, in the operating characteristic diagram shown in FIG. 4, when the flow rate control valve 11 starts operating, the secondary pressure is at point A, and after that, that is, after the operating time of the time signal generator 15 ends, it is at point A. When the energization amount is decreased from , point B is reached, and the predetermined 2
Next pressure P B is obtained. Next, when the amount of current is increased from point B, point C is reached. Further, when the energization amount is reduced from the energization amount at this point and set to the minimum energization amount I L , a point D is reached, and a predetermined secondary pressure lower than the above-mentioned secondary pressure P B is obtained. The minor loop when the amount of current is further increased from point D is at point
Intersects the main loop (X-A) at C'.

この点C′からまた通電量を減少させて行くと
上記点Dよりさらに下にさがつてしまい上記2次
圧PDよりも低い圧力になつてしまうが、制御
上、通電量を点C′に対応する値までとするので
はなくさらにそれよりも大きい上記点Cに至る値
まで増大させてから減少させる場合においては点
Cから先の点Dに至るマイナーループの軌跡をと
ることになる。
If the amount of energization is decreased again from this point C', it will go further below the point D and the pressure will be lower than the secondary pressure P D , but for control purposes, the amount of energization should be reduced to point C'. If the value is not increased up to a value corresponding to , but is increased to a value that reaches point C, which is larger than that, and then decreased, a minor loop trajectory from point C to point D will be taken.

従つて点Dに至つたあとは点Cまで通電量を増
大させたのち通電量を減少させれば最小通電量I
Lのときには必ず点Dに戻り、所定の2次圧PD
得られることになる。
Therefore, after reaching point D, increase the energization amount to point C and then decrease the energization amount to obtain the minimum energization amount I.
When the pressure is L , the pressure always returns to point D, and a predetermined secondary pressure P D is obtained.

従つてこの2次圧PDを上記下限2次圧P2Lに
設定しておけば最小通電量ILでは必ず下限2次
圧P2Lが得られることになる。
Therefore, if this secondary pressure P D is set to the lower limit secondary pressure P 2 L, the lower limit secondary pressure P 2 L will always be obtained with the minimum amount of current I L.

つまり、一度最大通電量IMまで通電した後に
通電量を増減しても、最小通電量ILにおける下
限次圧P2Lは一定値を得ることができることにな
り、燃焼装置のバーナーは逆火されることがな
い。また、2次圧の制御幅を拡大することができ
る。
In other words, even if the energization amount is increased or decreased after the energization reaches the maximum energization amount I M , the lower limit next pressure P 2 L at the minimum energization amount I L can be maintained at a constant value, and the burner of the combustion device will not backfire. never be done. Moreover, the control width of the secondary pressure can be expanded.

なお、上記実施例において、時限信号発生器1
5の設定時間は最大通電量IMで電磁石の磁路が
完全に磁化(磁区が整磁)される時間を必要とす
る。さらに、本発明は電磁石への通電量を制御し
て吐出2次圧を制御できる流量制御弁に広く適用
でき、吸入1次圧の変動に拘わることなく所定の
吐出2次圧を制御できる流量制御弁に限定される
ものでない。
Note that in the above embodiment, the time signal generator 1
The set time 5 requires a time for the magnetic path of the electromagnet to be completely magnetized (the magnetic domain is demagnetized) at the maximum energization amount I M. Furthermore, the present invention can be widely applied to flow control valves that can control secondary discharge pressure by controlling the amount of electricity supplied to electromagnets, and can control flow rate control that can control a predetermined secondary discharge pressure regardless of fluctuations in primary suction pressure. It is not limited to valves.

以上のように、本発明は電磁石を備えた流量制
御弁の電磁石への通電量を、検出手段からの制御
信号により増減制御させて流量制御弁の吐出2次
圧を制御するようにした流量制御弁の制御装置に
おいて、電磁石への通電開始時から最大通電量で
電磁石の磁路が完全に磁化される時間まで、その
電磁石が上記制御信号により通電量を増減制御さ
れるのを禁止し電磁石へ所定の上限吐出2次圧を
得るための最大通電量を与える所定の時限信号を
発生する時限信号発生器を設けたものであるた
め、電磁石への通電電開始に際して設定時間上限
2次圧を与える最大通電量を通電させて、電磁石
の磁路を完全に磁化させた後、該電磁石への通電
量を増減させることにより流量制御弁の吐出2次
圧を制御できることから、上記最大通電量に応じ
た電磁石の保磁力により通電量を増減しても最大
通電量における下限2次圧が常に一定値を得るこ
とができるマイナーループを確立できることにな
り、2次圧の制御幅を拡大できるという効果を奏
する。
As described above, the present invention provides a flow control system that controls the discharge secondary pressure of the flow control valve by increasing or decreasing the amount of current applied to the electromagnet of the flow control valve equipped with an electromagnet, using a control signal from the detection means. In a valve control device, the electromagnet is prohibited from being controlled to increase or decrease the energization amount by the above control signal from the time when energization to the electromagnet starts until the time when the magnetic path of the electromagnet is completely magnetized at the maximum energization amount. Since it is equipped with a timed signal generator that generates a predetermined timed signal that gives the maximum amount of energization to obtain a predetermined upper limit discharge secondary pressure, the upper limit secondary pressure is given for a set time when energization starts to the electromagnet. After the magnetic path of the electromagnet is completely magnetized by applying the maximum amount of current, the discharge secondary pressure of the flow control valve can be controlled by increasing or decreasing the amount of current applied to the electromagnet. Due to the coercive force of the electromagnet, it is possible to establish a minor loop in which the lower limit secondary pressure at the maximum energization amount can always obtain a constant value even if the amount of energization is increased or decreased.This has the effect of expanding the control width of the secondary pressure. play.

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

第1図は本発明の制御装置を適用した流量制御
弁の構成を示す図、第2図は第1図の動作特性
図、第3図は本発明の一実施例による流量制御弁
の制御装置を示すブロツク図、第4図は第3図の
動作特性図である。 5は電磁石、11は流量制御弁、15は時限信
号発生器、IMは最大通電量、P2Lは下限2次
圧。
FIG. 1 is a diagram showing the configuration of a flow control valve to which the control device of the present invention is applied, FIG. 2 is an operating characteristic diagram of FIG. 1, and FIG. 3 is a flow control valve control device according to an embodiment of the present invention. FIG. 4 is a block diagram showing the operating characteristics of FIG. 3. 5 is an electromagnet, 11 is a flow control valve, 15 is a time signal generator, I M is the maximum amount of current, and P 2 L is the lower limit secondary pressure.

Claims (1)

【特許請求の範囲】 1 電磁石を備えた流量制御弁の電磁石への通電
量を、検出手段からの制御信号により増減信号に
より増減制御させて流量制御弁の吐出2次圧を制
御するようにした流量制御装置において、電磁石
への通電開始時から最大通電量で電磁石の磁路が
完全に磁化される時間まで、その電磁石が上記制
御信号により通電量を増減制御されるのを禁止し
電磁石へ所定の上限吐出2次圧を得るための最大
通電量を与える所定の時限信号を発生する時限信
号発生器を設けたことを特徴とする流量制御弁の
制御装置。 2 検出手段は温度検出装置であつて、温度に応
じた制御信号を電磁石に与えて流量制御弁の吐出
2次圧を制御することを特徴とする特許請求の範
囲第1項に記載の流量制御弁の制御装置。
[Claims] 1. The amount of current applied to the electromagnet of a flow control valve equipped with an electromagnet is increased or decreased by an increase/decrease signal from a detection means, thereby controlling the discharge secondary pressure of the flow control valve. In a flow rate control device, the amount of energization of the electromagnet is prohibited from being increased or decreased by the above control signal from the time when energization starts to the electromagnet until the time when the magnetic path of the electromagnet is completely magnetized at the maximum amount of energization, and the amount of energization of the electromagnet is prohibited 1. A control device for a flow rate control valve, comprising a time signal generator that generates a predetermined time signal that provides a maximum amount of current to obtain an upper limit discharge secondary pressure. 2. Flow rate control according to claim 1, wherein the detection means is a temperature detection device, and controls the discharge secondary pressure of the flow rate control valve by giving a control signal according to the temperature to an electromagnet. Valve control device.
JP13807578A 1978-11-07 1978-11-07 Control device for flow control valve Granted JPS5563074A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13807578A JPS5563074A (en) 1978-11-07 1978-11-07 Control device for flow control valve

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13807578A JPS5563074A (en) 1978-11-07 1978-11-07 Control device for flow control valve

Publications (2)

Publication Number Publication Date
JPS5563074A JPS5563074A (en) 1980-05-12
JPS6134029B2 true JPS6134029B2 (en) 1986-08-05

Family

ID=15213371

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13807578A Granted JPS5563074A (en) 1978-11-07 1978-11-07 Control device for flow control valve

Country Status (1)

Country Link
JP (1) JPS5563074A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP4802262B2 (en) * 2009-02-17 2011-10-26 ジヤトコ株式会社 Hydraulic control device

Also Published As

Publication number Publication date
JPS5563074A (en) 1980-05-12

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