Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPS5855647B2 - temperature compensated solenoid - Google Patents
[go: Go Back, main page]

JPS5855647B2 - temperature compensated solenoid - Google Patents

temperature compensated solenoid

Info

Publication number
JPS5855647B2
JPS5855647B2 JP10514478A JP10514478A JPS5855647B2 JP S5855647 B2 JPS5855647 B2 JP S5855647B2 JP 10514478 A JP10514478 A JP 10514478A JP 10514478 A JP10514478 A JP 10514478A JP S5855647 B2 JPS5855647 B2 JP S5855647B2
Authority
JP
Japan
Prior art keywords
solenoid
winding
temperature
resistance
magnetomotive force
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
JP10514478A
Other languages
Japanese (ja)
Other versions
JPS5533042A (en
Inventor
雅文 綱田
豪夫 山本
昭 川村
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.)
Shibaura Machine Co Ltd
Original Assignee
Toshiba Machine Co Ltd
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 Toshiba Machine Co Ltd filed Critical Toshiba Machine Co Ltd
Priority to JP10514478A priority Critical patent/JPS5855647B2/en
Publication of JPS5533042A publication Critical patent/JPS5533042A/en
Publication of JPS5855647B2 publication Critical patent/JPS5855647B2/en
Expired legal-status Critical Current

Links

Landscapes

  • Magnetically Actuated Valves (AREA)

Description

【発明の詳細な説明】 本発明は比例制御用ソレノイドに係り、特に励磁巻線の
温度上昇に伴なう起磁力の低下を補償するようにしたソ
レノイドに関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a proportional control solenoid, and more particularly to a solenoid that compensates for a decrease in magnetomotive force caused by an increase in the temperature of an excitation winding.

従来、比例層IJ御用ソレノイドはジョイスティック(
可変抵抗器の一種)と結合して建設機械などにおいて連
続通電にて使用されることが多く、通電による励磁巻線
の温度上昇は無視できない程大きくなり、このため巻線
抵抗の増大をきたし、バッテリなどの定電圧電源を用い
ていると結局駆動電流が低下し、起電力が小さくなり例
えばソレノイド力による油圧弁の制御においては出力流
体が低減されその影響は多大である。
Conventionally, the proportional layer IJ solenoid was a joystick (
It is often used in conjunction with a variable resistor (a type of variable resistor) in continuous energization in construction machinery, etc., and the temperature rise in the excitation winding due to energization becomes so large that it cannot be ignored, resulting in an increase in the winding resistance. If a constant voltage power source such as a battery is used, the drive current will eventually decrease, and the electromotive force will become smaller. For example, when controlling a hydraulic valve using a solenoid force, the output fluid will be reduced, which has a significant effect.

そこで本発明は温度上昇に因づく起磁力の低下を補償す
るため励磁巻線に負の温度係数を有する抵抗素子を直列
に接続した新規なソレノイドを提供せんとするものであ
る。
Therefore, the present invention aims to provide a novel solenoid in which a resistance element having a negative temperature coefficient is connected in series to the excitation winding in order to compensate for the decrease in magnetomotive force due to temperature rise.

以下本発明の実施例を図面により説明する。Embodiments of the present invention will be described below with reference to the drawings.

第1図は本発明による二方向ソレノイドの縦断面図であ
って1,2はそれぞれ左右に設置された固定鉄心であり
この固定鉄心1,2は円筒状継鉄3と嵌着されている。
FIG. 1 is a longitudinal cross-sectional view of a two-way solenoid according to the present invention, and numerals 1 and 2 are fixed iron cores installed on the left and right sides, respectively, and these fixed iron cores 1 and 2 are fitted with a cylindrical yoke 3.

4,4Aは可動鉄心6を軸方向に摺動可能に支承する軸
受で同軸受4,4Aと固定鉄、し1,2との間にはそれ
ぞれ非磁性体のブツシュ5,5Aが装着されておりこれ
により軸受4,4Aを磁気的に遮断している。
4 and 4A are bearings that support the movable iron core 6 so as to be slidable in the axial direction, and non-magnetic bushings 5 and 5A are installed between the bearings 4 and 4A and the fixed irons 1 and 2, respectively. This magnetically isolates the bearings 4, 4A.

7.7Aは可動鉄心6が固定鉄心1,2に吸着するのを
防止する非磁性体スペーサである。
7.7A is a non-magnetic spacer that prevents the movable core 6 from adhering to the fixed cores 1 and 2.

継鉄3の中央内側突出部3Aと固定子1,2とで形成さ
れる空間にはコイル巻枠8,8Aが配設されておりこれ
に励磁巻線9,9Aがそれぞれ巻回されている。
Coil winding frames 8, 8A are arranged in the space formed by the central inner protrusion 3A of the yoke 3 and the stators 1, 2, and excitation windings 9, 9A are wound around these, respectively. .

10 、1 OAは前記励磁巻線9,9Aとそれぞれ巻
回方向が等しく且つ並列となるように接続された励磁巻
線であって起磁力に関しては励磁巻線9と10(又は9
Aと1 OA)による起磁力の加算されたものがソレノ
イド出力となるように構成されている。
10 and 1 OA are excitation windings connected so that the winding directions are the same and parallel to the excitation windings 9 and 9A, respectively, and the excitation windings 9 and 10 (or 9
The structure is such that the sum of the magnetomotive forces caused by A and 1 OA) becomes the solenoid output.

尚励磁巻線9,10と9A、10Aへの通電はそれぞれ
別々に行わ几可動鉄心6は左方、右方へとスプリング1
2,12Aに抗して所定のバランス位置まで位動される
ようになっている。
The excitation windings 9, 10, 9A, and 10A are energized separately, and the movable iron core 6 moves leftward and rightward to the spring 1.
2, 12A to a predetermined balance position.

11.11Aはサーミスタであってそれぞれ励磁巻線1
0.1OAに直列接続されている。
11.11A are thermistors, each with excitation winding 1
Connected in series to 0.1OA.

第2図は第1図の左方の励磁巻線9,10とサーミスタ
11の接続を示すものでR1,R2は励磁巻線9.10
の抵抗値を示す。
Figure 2 shows the connection between the excitation windings 9 and 10 on the left side of Figure 1 and the thermistor 11, and R1 and R2 are the excitation windings 9 and 10.
shows the resistance value.

R3はサーミスタ11の抵抗値を示す。R3 indicates the resistance value of the thermistor 11.

VRはジョイスティック可変抵抗器の1部で励磁巻線9
へ0通電電流の設定部である。
VR is part of the joystick variable resistor and excitation winding 9
This is a setting section for setting the 0 current to 0.

第3図は従来のソレノイドの接続回路であってR4は励
磁巻線の抵抗値を示す。
FIG. 3 shows a conventional solenoid connection circuit, and R4 indicates the resistance value of the excitation winding.

第4図は温度上昇に際して温度補償をしていない従来の
ソレノイドの特性変化(破線)と本発明による温度補償
型ソレノイドの特性変化(実線)とを併記したものであ
る。
FIG. 4 shows the change in characteristics of a conventional solenoid without temperature compensation (broken line) and the change in characteristics of the temperature-compensated solenoid according to the present invention (solid line) when the temperature rises.

同図について説明すると従来のソレノイドにおいては例
えば温度10の状態からtl、t2へと上昇するに従い
抵抗R4は増加し、定電圧電源■により電流■は逆に減
少する傾向となる。
To explain this figure, in the conventional solenoid, as the temperature increases from, for example, 10 to tl and t2, the resistance R4 increases, and the constant voltage power supply (2) causes the current (2) to decrease.

又それにより起磁力(NI:巻数×電流)も落ち込み、
ソレノイドの出力性能は低下する。
As a result, the magnetomotive force (NI: number of turns x current) also decreases,
The output performance of the solenoid decreases.

起磁力の設計にあたっては許容される温度範囲の中間の
温度に稜いて設計計算されるので今の例では温度t1に
おける起磁力をもって定格ということになる。
When designing the magnetomotive force, the design calculation is performed at a temperature in the middle of the allowable temperature range, so in this example, the magnetomotive force at the temperature t1 is the rated value.

その定格起磁力の線を記号■で表わせばt1〜t2の温
度範囲では■以下となり、ソレノイド出力は定格値に対
し不足し、最高出力は低下し例えばクレーンなどの捲き
上げ、捲き下げ等の速度が落込み操作性能が悪化するこ
とにもなる。
If the line of the rated magnetomotive force is represented by the symbol ■, it will be less than ■ in the temperature range from t1 to t2, the solenoid output will be insufficient for the rated value, and the maximum output will decrease, for example, the speed of hoisting and hoisting of cranes etc. However, this will also lead to deterioration in operational performance.

しかるに本発明による温度補償の方式によると実線に示
すように起磁力の落込みは大巾に改善されることになる
However, according to the temperature compensation method according to the present invention, the drop in magnetomotive force is greatly improved as shown by the solid line.

次に第3図について抵抗の温度上昇による変化の様子を
分析してみる。
Next, let's analyze the change in resistance due to temperature rise in Figure 3.

以下の例では可変抵抗器の部分の抵抗は省略して考える
In the following example, the resistance of the variable resistor will be omitted.

第3図の全抵抗Rは(温7度toでR1,R2゜R3と
する) 温度上昇による抵抗値の増分1JR1,JR2゜JR3
とするとt2における各抵抗値R1’、 R2’。
The total resistance R in Figure 3 is (assumed to be R1, R2°R3 at a temperature of 7°C).The increase in resistance value due to temperature rise is 1JR1, JR2°JR3.
Then, each resistance value R1', R2' at t2.

R3’は 励磁巻線10の抵抗R2とサーミスタ11の抵抗R3の
和は温度上昇によりR2午R3’<R2+R3となる。
R3' is the sum of the resistance R2 of the excitation winding 10 and the resistance R3 of the thermistor 11, which becomes R2<R3'<R2+R3 due to the temperature rise.

この傾向を利用して励磁巻線9の抵抗R1の温度上昇に
伴う電流値■1の減少による起磁力の低下分を励磁巻線
10へ流れる電流I2の増加によって補完しようとする
ものである。
Utilizing this tendency, an attempt is made to compensate for the decrease in magnetomotive force due to a decrease in current value (1) due to a rise in temperature of resistor R1 of excitation winding 9 by increasing current I2 flowing to excitation winding 10.

このように並列回路を構成したのはサーミスタの通電々
流容量が比較的少ないため第3図の励磁巻線に直列にサ
ーミスタを接続する方式では起磁力に必要な電流値を確
保できないという理由がある。
The reason for configuring the parallel circuit in this way is that the current carrying capacity of the thermistor is relatively small, so the method of connecting the thermistor in series with the excitation winding shown in Figure 3 cannot secure the current value necessary for the magnetomotive force. be.

又励磁巻線、サーミスタを含む合成抵抗値を温度変化が
あっても一定に抑えて起磁力の外部指令手段としての可
変抵抗器VRの値に対し指令電流値 l−11+I2が
1:1に対応する必要があるからである。
In addition, the combined resistance value including the excitation winding and thermistor is held constant even if there is a temperature change, and the command current value 1-11 + I2 corresponds 1:1 to the value of the variable resistor VR, which serves as an external command means for magnetomotive force. This is because it is necessary.

1つの実施例としての数値を示すと となりはゾ合威抵抗R1電流■は一定となっている。Showing numerical values as one example: Next to it, the resistance R1 current ■ is constant.

以上説明したように本発明においてはソレノイドの励磁
巻線を二つの部分に分けてその1方の巻線部分に直列に
サーミスタを接続して補償回路を構成し、他方の巻線部
分をそれらと並列に接続しておりこれら部分巻線の抵抗
値及びサーミスタの抵抗温度特性を適切に選択すること
によって温度変化があっても起磁力変化の少ないソレノ
イドを形成することが可能となった。
As explained above, in the present invention, the excitation winding of a solenoid is divided into two parts, a thermistor is connected in series to one of the winding parts to form a compensation circuit, and the other winding part is connected to the two parts. By appropriately selecting the resistance values of these partial windings connected in parallel and the resistance-temperature characteristics of the thermistor, it has become possible to form a solenoid with little change in magnetomotive force even when temperature changes.

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

第1図は本発明による二方向ソレノイドの要部縦断面図
、第2図は第1図の左方側ソレノイドの回路接続図、第
3図は従来のソレノイドの回路接続図、第4図は温度変
化に対する起磁力、電流及び抵抗値の変化を示すグラフ
である。 1.2・・・・・・固定鉄心、3・・・・・・継矢、4
・・・・・・軸受、5・・・・・・ブツシュ、6・・・
・・・可動鉄心、7・・・・・・スペーサ、8・・・・
・・巻枠、9,10・・・・・・励磁巻線、11・・・
・・・サーミスタ。
Fig. 1 is a longitudinal cross-sectional view of the essential parts of the two-way solenoid according to the present invention, Fig. 2 is a circuit connection diagram of the left side solenoid in Fig. 1, Fig. 3 is a circuit connection diagram of a conventional solenoid, and Fig. 4 is It is a graph showing changes in magnetomotive force, current, and resistance value with respect to temperature changes. 1.2... Fixed iron core, 3... Connector, 4
...Bearing, 5...Button, 6...
...Movable iron core, 7...Spacer, 8...
... Winding frame, 9, 10... Excitation winding, 11...
...Thermistor.

Claims (1)

【特許請求の範囲】[Claims] 1 定電圧直流電源に接続される励磁巻線への通電電流
を変化させて起磁力を制御するようにしたソレノイドに
おいて、前記励磁巻線を第1.第2の巻線部分に区分け
すると共に、前記第1の巻線に対し、第2の巻線と負の
温度係数を有する抵抗素子との直列接続により構成した
補償回路を並列に接続形成したことを特徴とする温度補
償型ソレノイド。
1. In a solenoid that controls magnetomotive force by changing the current flowing to an excitation winding connected to a constant voltage DC power supply, the excitation winding is connected to a first. It is divided into a second winding part, and a compensation circuit configured by a series connection of the second winding and a resistance element having a negative temperature coefficient is connected in parallel to the first winding. A temperature compensated solenoid featuring:
JP10514478A 1978-08-29 1978-08-29 temperature compensated solenoid Expired JPS5855647B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10514478A JPS5855647B2 (en) 1978-08-29 1978-08-29 temperature compensated solenoid

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10514478A JPS5855647B2 (en) 1978-08-29 1978-08-29 temperature compensated solenoid

Publications (2)

Publication Number Publication Date
JPS5533042A JPS5533042A (en) 1980-03-08
JPS5855647B2 true JPS5855647B2 (en) 1983-12-10

Family

ID=14399534

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10514478A Expired JPS5855647B2 (en) 1978-08-29 1978-08-29 temperature compensated solenoid

Country Status (1)

Country Link
JP (1) JPS5855647B2 (en)

Families Citing this family (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5788411A (en) * 1980-11-21 1982-06-02 Fujitsu Ltd Forming method of optical waveguide
JPS58178303A (en) * 1982-04-14 1983-10-19 Fujitsu Ltd Formation of optical waveguide
JPS58190903A (en) * 1982-05-04 1983-11-08 Oki Electric Ind Co Ltd Formation of optical waveguide
JPH0723927B2 (en) * 1983-08-09 1995-03-15 富士通株式会社 Method of manufacturing optical waveguide
JPS6034163U (en) * 1983-08-16 1985-03-08 株式会社 小金井製作所 high speed solenoid valve
US4536728A (en) * 1983-10-03 1985-08-20 International Telephone & Telegraph Corp. Valve solenoid windings
JPH0697286B2 (en) * 1985-07-23 1994-11-30 日本電気株式会社 Optical circuit and manufacturing method thereof
JP2010074013A (en) * 2008-09-22 2010-04-02 Toyooki Kogyo Kk Electromagnet apparatus

Also Published As

Publication number Publication date
JPS5533042A (en) 1980-03-08

Similar Documents

Publication Publication Date Title
US4517483A (en) Permanent magnet rotor with saturable flux bridges
US5422525A (en) Switched reluctance machine having unbalance forces compensation coils
US4164722A (en) Electromagnetic actuator with torque-compensating poles
JPS5855647B2 (en) temperature compensated solenoid
IE801714L (en) Electric machine
KR101118337B1 (en) Magnetic flux distribution control type rotary electrical machine system
US2629847A (en) Magnetic amplifier circuits for applying reversible direct-current voltage to inductive loads
US2305937A (en) Regulating system
US9209663B2 (en) Apparatus and methods for passive magnetic reduction of thrust force in rotating machines
US4387330A (en) Balanced single phase alternating current induction motor
US11215226B2 (en) Stray flux compensation in a magnetic bearing device
JP2013137067A (en) Magnetic bearing
CN116733846A (en) Suspension force symmetrical six-pole constant current source excitation electromagnetic bearing and design method thereof
JPH0544609B2 (en)
JPS6319726B2 (en)
US2456982A (en) Motor control
US2538119A (en) Electrical control system
KR940002921B1 (en) Method of controlling servo motor
JP2010130870A (en) Winding field type motor, and control method thereof
US2934689A (en) Servo systems and quadrature signal filter therefor
JP7309693B2 (en) Electric motor and winding method
SU847478A1 (en) Electric drive
US2912631A (en) Dynamoelectric machinery having a supplemental saturable core rotor
CN116365816B (en) 6/4-pole bearingless doubly salient sheet motor with parallel structure and suspension control method thereof
JP2542491Y2 (en) Linear motor