JPS5948903A - Electromagnet device - Google Patents

Electromagnet device

Info

Publication number
JPS5948903A
JPS5948903A JP57159874A JP15987482A JPS5948903A JP S5948903 A JPS5948903 A JP S5948903A JP 57159874 A JP57159874 A JP 57159874A JP 15987482 A JP15987482 A JP 15987482A JP S5948903 A JPS5948903 A JP S5948903A
Authority
JP
Japan
Prior art keywords
power supply
electromagnetic coil
brake
power source
voltage
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
JP57159874A
Other languages
Japanese (ja)
Inventor
Masumi Kanbe
神戸 真澄
Masami Nomura
正実 野村
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.)
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 JP57159874A priority Critical patent/JPS5948903A/en
Publication of JPS5948903A publication Critical patent/JPS5948903A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F7/00Magnets
    • H01F7/06Electromagnets; Actuators including electromagnets
    • H01F7/08Electromagnets; Actuators including electromagnets with armatures
    • H01F7/18Circuit arrangements for obtaining desired operating characteristics, e.g. for slow operation, for sequential energisation of windings, for high-speed energisation of windings
    • H01F7/1805Circuit arrangements for holding the operation of electromagnets or for holding the armature in attracted position with reduced energising current

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Braking Arrangements (AREA)

Abstract

PURPOSE:To omit the series resistor of a circuit, and to reduce power consumption by first energizing an electromagnetic coil by a first power supply at high DC voltage and operating an operating section and changing over the first power supply to a second power supply at low DC voltage and energizing the coil. CONSTITUTION:The circuit for the hoisting machine of an elevator is constituted by connecting a series circuit of a changeover means 13 consisting of a brake contact, a control contact 21 and the electromagnetic coil 12 between the plus terminal and minus terminal of the first power supply 30 generating high DC voltage. The second power supply 31 generating DC voltage lower than the power supply 30 is set up in addition to the circuit, and the plus terminal of the power supply 31 is connected to a node between the changeover means 13 and the control contact 21 through a rectifying diode 32, which is reverse-connected to the power supply 30 and forward-connected to the power supply 31. The minus terminal of the power supply 31 is connected to a node between the control contact 21 and the coil 12 throgh a parallel resistor 2 and a diode for discharge reverse-connected to either of the power supplies 30 and 31.

Description

【発明の詳細な説明】 この発明は直流電源で付勢される電磁石装置に係り、特
にその制御に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an electromagnetic device powered by a DC power source, and particularly to its control.

電磁石は、電磁コイルを付勢して吸引力を発生させ、こ
の吸引力で作動部を作動させて所定の動作を行わせるも
ので、ブレーキ、クラッチ及び電気回路全開閉する接触
器等に多用されている。
Electromagnets generate an attractive force by energizing an electromagnetic coil, and this attractive force operates an actuating part to perform a predetermined operation, and is often used in brakes, clutches, and contactors that fully open and close electric circuits. ing.

第1図は電磁石が使用されたエレベータの巻上機を示し
9図において、(1)は本体、(2)はこの本体(1)
に軸支されたりな車、(3)はこのつな車(2)に回転
力を伝える回転軸、(4)はこの回転軸(3)に取り付
けられたブレーキ車、(51Hこのブレーキ車(4)全
把持して制動させる一対のブレーキシュー、(61i下
端部が軸(6a)を介して回動自在に本体(1)K取り
付けられ、中間部に軸(6b)’i+−介してブレーキ
シュー(5)がそれぞれ取り付けられて立設された一対
のブレーキレバー、(7)は一端が本体(1)に固定さ
れ、それぞれブレーキレバー(6)の上端部を遊貫して
水平方向に延在する一対のブレーキロンド、(8)はこ
のブレーキロンド(7)の他端にそれぞれ係止されてブ
レーキレバー(6)ヲ第1図の入方向へ常時押している
一対のブレーキばね、(9)はL字状に形成され、M曲
部で軸(9a)’e介して本体(1)九回動自在に取り
付けられた一対のカムからなる作動部で、それぞれ上記
り字の一辺がブレーキレバー(6)に固設された突起部
(1Gに当接されている。Uは本体(11の上部を遊貫
し立設されて上下動可能な磁性体からなるプランジャで
、下面がカム(9)の他辺端に当接して常時上方へ押し
上げられている。a’au本体(1)内に収納され、プ
ランジャa9に遊具された管状の電磁コイルで、直流電
源で付勢されてプランジャUt−吸引し、下方へ移動さ
せるもので、上記プランジャ(Lllと共沈電磁石(1
2A)を構成している。a3はプランジャO2が上方に
あるとき電気回路を閉成し、下方にあるとき開放するブ
レーキ接点からなる切換手段である。
Figure 1 shows an elevator hoisting machine that uses electromagnets, and in Figure 9, (1) is the main body, and (2) is the main body (1).
(3) is a rotating shaft that transmits rotational force to this connecting wheel (2), (4) is a brake wheel attached to this rotating shaft (3), (51H this brake wheel ( 4) A pair of brake shoes that fully grip and apply braking, (61i's lower end is rotatably attached to main body (1)K via shaft (6a), and brake is attached to the middle part via shaft (6b)'i+- A pair of brake levers (7) each have a shoe (5) attached thereto and stand upright; one end of the brake lever (7) is fixed to the main body (1), and each extends horizontally through the upper end of the brake lever (6). A pair of brake ronds (8) are attached to the other ends of the brake ronds (7), and a pair of brake springs (9) are respectively engaged with the other ends of the brake ronds (7) and constantly push the brake lever (6) in the inward direction as shown in FIG. is formed into an L-shape, and is an actuating part consisting of a pair of cams that are rotatably attached to the main body (1) through shafts (9a)'e at the M-curved part, and one side of the above-mentioned letter is the brake lever. (6) is in contact with the protrusion (1G). U is a plunger made of a magnetic material that freely passes through the upper part of the main body (11) and is movable up and down. ) is constantly pushed upward by contacting the other side end of the a'au body (1).It is a tubular electromagnetic coil that is housed in the a'au body (1) and is attached to the plunger a9, and is energized by a DC power source to move the plunger Ut. - It is a device that attracts and moves it downward, and it is a coprecipitating electromagnet (1) with the plunger (Lll).
2A). A3 is a switching means consisting of a brake contact which closes an electric circuit when the plunger O2 is in the upper position and opens it when the plunger O2 is in the lower position.

すなわち、電磁コイルazが消勢されているときは、ブ
レーキレバー(6)はブレーキばね(8)によって第1
図の入方向へ押され、突起部(lIk介してカム(9)
ヲ第1図のB方向へ回転書せてプランジャa11i押し
上げると共に、ブレーキシュー(5)でブレーキ車(4
)全把持して回転軸(3)全制止させ、つな車(2)の
回転を止めるものである。
That is, when the electromagnetic coil az is deenergized, the brake lever (6) is moved to the first position by the brake spring (8).
The cam (9) is pushed in the direction shown in the figure, and the cam (9)
Rotate in direction B in Figure 1 to push up the plunger a11i, and use the brake shoe (5) to release the brake wheel (4).
) to completely stop the rotating shaft (3) and stop the rotation of the hitch wheel (2).

次に、電磁コイル0zが付勢されると、プランジャUa
吸引されてカム(9)ヲ第1図のC方向へ回転させてブ
レーキばね(8)に抗してブレーキレバー(6)を第1
図のC方向へ移動させる。このため、ブレーキシュー(
5)はブレーキ車(4)を解放して制動状態を解く。
Next, when the electromagnetic coil 0z is energized, the plunger Ua
The cam (9) is attracted and rotated in the direction C in Figure 1, and the brake lever (6) is moved to the first position against the brake spring (8).
Move in direction C in the figure. For this reason, the brake shoe (
5) releases the brake wheel (4) to release the braking state.

ここで、電磁コイルaりはプランジャαυを吸引しカム
(9)全作動させた状態に保持するのに要する付勢力に
比べてプランジャUt吸引してカム(91k 作mむさ
せようとするときは大きな付勢力を必要とするものであ
る。t′のため、直流の電磁コイルQ3が使用される場
合は、カム(9)を作動させるときに高い電圧が印加さ
れ9作動後は抵抗によって降圧された電圧が印加される
よう構成されていた0第2図は第1図のエレベータの巻
上様に使用された従来の電磁石装置を示す。図中、第1
図と同一符号は同−又は相当部分を示し、cAは電磁コ
イルQりの定格電圧エリも高い電圧値Eボルトヲ出力す
る直流電源、aは制御装置(図示しない)によって開閉
される制御接点で、一端が直流電源(イ)のプラス端子
に接続され、他端がブレーキ接点0の一端に接続されて
いる。(ハ)は抵抗値Rpヲ有し。
Here, compared to the urging force required to attract the plunger αυ and keep the cam (9) fully activated, the electromagnetic coil a is larger than the urging force required to attract the plunger Ut and make the cam (91k) operate. This requires a large biasing force.Because of t', when a DC electromagnetic coil Q3 is used, a high voltage is applied when the cam (9) is operated, and after the cam (9) is operated, the voltage is lowered by the resistor. Figure 2 shows a conventional electromagnetic device used for hoisting the elevator shown in Figure 1.
The same reference numerals as in the figure indicate the same or equivalent parts, cA is a DC power supply that outputs a voltage value E volts which is also higher than the rated voltage area of the electromagnetic coil Q, a is a control contact that is opened and closed by a control device (not shown), One end is connected to the positive terminal of the DC power supply (a), and the other end is connected to one end of the brake contact 0. (c) has a resistance value Rp.

電磁コイルα力に並列に接続された並列抵抗、(ハ)は
ブレーキ接点0りに並列に接続され、かつ、電磁コイル
(I21と並列抵抗c!邊とからなる並列回路を介して
直流電源(至)のマイナス店14子に接続された直列抵
抗で、電磁コイル圓に所定の電圧が印加されるように抵
抗値IRQに設定されている。
A parallel resistor (c) connected in parallel to the electromagnetic coil α force is connected in parallel to the brake contact 0, and is connected to the DC power source (c) through a parallel circuit consisting of the electromagnetic coil (I21) and the parallel resistor c! A series resistor connected to the negative terminal 14 of (to) is set to a resistance value IRQ so that a predetermined voltage is applied to the electromagnetic coil circle.

上記のとおジ構成された電磁石装置において。In an electromagnetic device configured as above.

制御接点CDが開放されていると、電磁コイルOzは消
勢されて巻上様を制動状態にする。一方、制御接点al
lが閉成されると、電磁コイル02 U fit −r
21)−tJ3−02−■の回路によって電圧値Eで付
勢され。
When the control contact CD is open, the electromagnetic coil Oz is deenergized and the hoist is placed in a braking state. On the other hand, control contact al
When l is closed, the electromagnetic coil 02 U fit -r
21)-tJ3-02-■ is energized with voltage value E by the circuit.

プランジャa9を吸引して巻上様の制動状態を解くと共
に、ブレーキ接点αjが開放されるので、!磁コイルO
zけ(イ)−(21)−(ハ)−(Iクー(イ)の回路
に切り換えられて付勢される。このため、直列抵抗□□
□が挿入され付勢力は減少これた値となる。次に、制御
接点12υが開放されると、!磁コイル(121ハ自身
に貯えられた電磁エネルギを並列抵抗(イ)を介して放
電して消勢され0巻上様を制動状態にする1、ところで
、上記電磁石装置では、並列抵抗−及びは動抵抗(ハ)
によって電力が消費されるため、電力を多く必要とする
ものであった。特に、並列抵抗Qal″iもともと?a
電磁コイル12に貯えられた電磁エネルギを放電させて
、制御接点(20が開放されたときの誘起電圧を抑える
ために設けらf’Lるものであるが、直列抵抗体勺が接
続された回路では、′?ば磁コイル(12の温度上昇に
よって電磁コイル(17Jにかかる電圧が上昇するのを
抑え、焼mを防ぐためにも使用されるものである。
At the same time as the plunger a9 is sucked to release the hoisting braking state, the brake contact αj is opened, so! Magnetic coil O
The circuit is switched and energized: zke(a)-(21)-(c)-(Iku(a)).For this reason, the series resistance □□
□ is inserted and the biasing force is reduced to the value. Next, when the control contact 12υ is opened, ! The electromagnetic energy stored in the magnetic coil (121) is discharged through the parallel resistor (1) and deenergized to bring the 0 winding into a braking state. Dynamic resistance (c)
This required a large amount of electric power. In particular, the parallel resistance Qal″i originally ?a
The electromagnetic energy stored in the electromagnetic coil 12 is discharged, and the control contact (f'L) is provided to suppress the induced voltage when the control contact (20) is opened. It is also used to suppress the voltage applied to the electromagnetic coil (17J) from increasing due to a rise in the temperature of the magnetic coil (12), and to prevent burnout.

すなわち。Namely.

VB : 電磁コイルQ2の印加電圧値RB:電磁コイ
ルO3の抵抗値 どし、第2図において、並列抵抗いの使用されない回路
でブレーキ接点αJが開放さt′L*とき、印加電圧値
VBは。
VB: Applied voltage value of electromagnetic coil Q2 RB: Resistance value of electromagnetic coil O3 In Fig. 2, when the brake contact αJ is opened t'L* in a circuit where the parallel resistor is not used, the applied voltage value VB is .

となる。一方電磁コイル(12VC並列抵抗(2つが接
続された回路では 一一一−−−−−−−−−−−−− ■と、なる。ここ
で、温度が上昇したとき、並列抵抗@及び直列抵抗(ハ
)は、温度係数が小さいので抵抗値RP及び工(sは不
変とし、抵抗値RBが増大したとすると、印加電圧値V
B9■式では電圧値Eに近すき、■式でn電圧値Eより
も低い電圧値RP、 E/’ (R8+RP)に近ずく
、Liがっ−r、温度上昇による抵抗値RBの変化に対
する印加?「正値vBへの影響は、並列抵抗(2りが接
μ°さ′i9ている方が小さい。この傾向ll−を抵抗
値R8及び■(1,が共1/C小さな値に設定される方
が顕著である1・このため。
becomes. On the other hand, when the electromagnetic coil (12 VC parallel resistance The resistance (C) has a small temperature coefficient, so if the resistance value RP and the resistance value (s) remain unchanged and the resistance value RB increases, the applied voltage value V
In formula B9, the voltage value RP is close to the voltage value E, and in the formula Impression? ``The influence on the positive value vB is smaller when the parallel resistance (2) is in contact with μ°'i9. 1.For this reason.

並列抵抗clり及び直列抵抗03で消費される電力は大
きな値となる欠点があった。
There was a drawback that the power consumed by the parallel resistor CL and the series resistor 03 was large.

この発明は上記欠点IC%みなされたものであり??j
+い直流電圧を有する第1の電源で電磁コイルを付勢し
て作動部を作動させ1作ルb後は上記第1の電源よりも
1氏い直流電圧の第2の電源に切り換え−C上記電磁コ
イルを付勢−するようにして、上記電磁コイルの回路の
直列抵抗を省いて〒1)゛力消費全減少させることを目
的どするものである3、第3図江この発明の一実施例で
、a(1図に示すエレベータの巻上様に実施した場合を
示す。図中第1図及び第2図と同一符号は同−又E1相
当部分を示し、 (1■はブレーキ接点からなる切換手
段、 C1lは高い直流電圧を有する第1の電源で、プ
ラス端子がブレーキ接点0し制御接点C11)を介して
電磁コイルHの一端に接続され、マイナス端子が電磁コ
イルazの他端に接続されている。口υは第1の電源(
至)よりも低い?「圧を有し、電磁コイルα7Jを連続
付勢可能な第2の電源で、マイナス端子が電磁コイルu
2の他端に接続されている。(嗜は第1の電源(7)に
対して逆接続さノ1.第2の′ζ源c11)に対して順
接続された整流ダイオードで、一端が第2の電源(+1
1のプラス端子に、他端がブレーキ接点(131と制御
接点シl)の間にそれぞれ接続されている。431は第
1の電源c1及び第2ρ電源c31)のいずノ1にも逆
接続された放′1b′用ダイオードで、一端が電磁コイ
ル(1邊の一端に、他端が並列抵抗(2)に接続されて
いる。
Is this invention considered to have the above drawback IC%? ? j
The electromagnetic coil is energized by the first power supply having a higher DC voltage to operate the actuating part, and after one cycle, the power supply is switched to the second power supply having a DC voltage higher than the first power supply -C. The purpose of the present invention is to energize the electromagnetic coil, omit the series resistance of the circuit of the electromagnetic coil, and thereby completely reduce power consumption. In the example, a (1) shows a case where the elevator is hoisted as shown in Fig. 1. In the figure, the same reference numerals as in Figs. 1 and 2 indicate the same parts or parts corresponding to E1, C1l is a first power supply having a high DC voltage, the positive terminal is connected to one end of the electromagnetic coil H via the brake contact 0 and the control contact C11), and the negative terminal is connected to the other end of the electromagnetic coil az. The port υ is connected to the first power supply (
lower than )? "The second power supply has a voltage that can continuously energize the electromagnetic coil α7J, and the negative terminal is connected to the electromagnetic coil u
It is connected to the other end of 2. (The rectifier diode is connected in reverse to the first power supply (7). The rectifier diode is connected forward to the second ′ζ source c11.
1, and the other end is connected between the brake contact (131 and control contact S1), respectively. 431 is a diode for radiation '1b' which is reversely connected to any one of the first power supply c1 and the second ρ power supply c31), and one end is connected to the electromagnetic coil (one end of one side), and the other end is connected to the parallel resistor (2 )It is connected to the.

上記のとおリイh成さ:hた電磁石装洒°叫おいて。As mentioned above, please refer to the electromagnet installation.

ブレーキ接心、a31が閉成されているとき、第1の電
源(至)、整流ダイオードGz及び第2の電源C(I)
’(1m介して閉回路が形成されるが、第1の?「源圓
は整流ダイオード(郁に1引上されているので第1の電
源体)から第2の’iIi 6’;’、 Chiの回路
に流れることはない。また第2の箱:j170+iは電
圧が圓いので第1の電源((財)へ流れることViない
ものである。
When the brake centroid, a31, is closed, the first power supply (to), the rectifier diode Gz and the second power supply C(I)
'(A closed circuit is formed through 1m, but the first source is the rectifier diode (the first power source because it is raised by 1) to the second 'iIi 6';', It does not flow to the circuit of Chi.The second box: j170+i has a round voltage, so Vi does not flow to the first power supply ((goods)).

今、制御接点C(1)が開放されているときけ電磁コイ
ルα2μ消勢されており1巻上様を制動状態にするO 次に、制御接点Q1)が閉成されると、市碍コイル(l
zけ(ト)−(lターQB−(12+−CIの回路によ
って第1の電源(7)で付勢され、プランジャ(lll
’i吸引してカム(91を作動させて巻上様の制動状態
を解く0また。プランジャ(Illの移動によってブレ
ーキ接点+13が開放されル+It’)で、電磁コイル
Htri CHI) −Cl2) −Cjl) −(1
21−Cl1)の回路へ切V換えられ、第2の電源61
)によって付勢さノする。第2の’ilf m C11
1の低電圧によ心付勢であっても*1aEFiコイル(
1っハブランジャ(+11(z吸引してカム(9)を作
動状態に保持するものである。凍た。
Now, when the control contact C(1) is open, the magnetic coil α2μ is deenergized and the first winding is in a braking state. Next, when the control contact Q1) is closed, the commercial coil α2μ is deenergized. (l
The plunger (llll) is energized by the first power supply (7) by the circuit of
'I sucks in the cam (91 to release the winding braking state. By moving the plunger (Ill), the brake contact +13 is released and the electromagnetic coil Htri CHI) -Cl2) - Cjl) −(1
21-Cl1), and the second power supply 61
). 2nd 'ilf m C11
*1aEFi coil (
1 hub plunger (+11 (z) is used to hold the cam (9) in the operating state. Freeze.

放電用ダイオード(至)によって阻止されているので並
列抵抗+aで電力が消費されることはない。
Since it is blocked by the discharge diode (to), no power is consumed by the parallel resistance +a.

次に、制御接点Qυが開放されると、電磁コイル(Ia
U自身に貯えられた電磁エネルギを並列抵抗(2乃及び
放電用ダイオード(ト)會介して放電し消勢されて巻上
様を制動状態にする、 第3図に示す実施例によれば、第1の電源c+tnで電
磁コイルazl付勢してプランジャα1)全吸引してカ
ム(9)を作動させ9巻上機の制動を解いた後、ブレー
キ接点θJで切り換えて低い電圧の第2の電源6υで?
ff 磁コイル0z1(付勢するようにしたので、電圧
?降下させるための直列抵抗を省くことができる一寸た
。並列抵抗(社)は電磁コイルqzの放電用として専用
できるので、放電用ダイオードG31によって電磁コイ
ルOzO伺勢状態における電力消費をなくすこともでき
るものである。更にまた。整流ダイオードGつを介して
第20電源01)を電磁コイルα2に接続したので、第
1の電源(至)がブレーキ接点(2)で開放されたとし
ても、電磁コイル021は連続して′通電されるもので
ある。
Next, when the control contact Qυ is opened, the electromagnetic coil (Ia
According to the embodiment shown in FIG. 3, the electromagnetic energy stored in U itself is discharged through a parallel resistor (2) and a discharging diode (T) and is deenergized to bring the hoist into a braking state. After energizing the electromagnetic coil azl with the first power supply c+tn and fully attracting the plunger α1), activating the cam (9) and releasing the brake on the hoisting machine 9, switch with the brake contact θJ to switch to the lower voltage second With 6υ power supply?
ff Magnetic coil 0z1 (Since it is energized, the series resistor for voltage drop can be omitted.The parallel resistor can be used exclusively for discharging the electromagnetic coil qz, so the discharge diode G31 It is also possible to eliminate power consumption when the electromagnetic coil OzO is in the waiting state.Furthermore, since the 20th power supply 01) is connected to the electromagnetic coil α2 via the rectifier diodes G, the first power supply (to) Even if the brake contact (2) is opened, the electromagnetic coil 021 is continuously energized.

なお、第2の電源は交流を整流して直流に変換する整流
体からなるものでもよく、このものによれは第3図の整
流ダイオードC(2を省略することができる。
Note that the second power source may be made of a rectifier that rectifies alternating current and converts it into direct current, and in this case, the rectifying diode C (2) in FIG. 3 can be omitted.

また、上記実施例では電磁コイルを付勢したときに巻上
様の制動状態全所くようにしたが、逆に常時制動状態が
解かれていて電磁コイルを付勢したときに制動状態にす
るものにもこの発明を利用できる。
In addition, in the above embodiment, when the electromagnetic coil is energized, all parts are in a winding-like braking state, but conversely, the braking state is always released, and when the electromagnetic coil is energized, the braking state is put in place. This invention can also be applied to things.

第4図は切換手段の他の実施例を示し0図中。FIG. 4 shows another embodiment of the switching means.

第3図と同一符号は同−又は相当部分を示す。図におい
て、(40は制御接点むυど同時l(閉成及び開放され
る補助制御接点、(Itmこの補助制御接点(41の閉
成によって付勢されて電磁コイルα邊がカム(9)全作
動させるのに必要な時間が少なくとも経過した後に常閉
接点(41a)を開放する時限リレーからなる時計手段
である。このものにあっても所期の目的を達することが
できると共に、電磁コイルO3の71i′ス回路に簡単
に組み込むことができる。
The same reference numerals as in FIG. 3 indicate the same or corresponding parts. In the figure, (40 is an auxiliary control contact which is closed and opened at the same time as the control contact υ), (Itm) is energized by the closing of this auxiliary control contact (41), and the electromagnetic coil α side is fully connected to the cam (9). This clock means consists of a time relay that opens the normally closed contact (41a) after at least the time required for activation has elapsed.Even with this, the intended purpose can be achieved, and the electromagnetic coil O3 It can be easily incorporated into the 71i' bus circuit.

ところで、上記説明では、この発明をエレベータの巻上
様に設けられた電磁ブレーキに使用する場合について述
べたが、その他の電磁石装置にも利用できるものである
1、 この発明は以上述べたとおり、高い直流電圧を有する第
1の’Ff源で電磁コイルを付勢し、この電磁コイルの
磁力で作動部全作動させた後、上記第1の電源よりも低
い直流電圧の第2の電源へ切換手段で切り換えて作動状
態を保持するようにしたので、直列抵抗によって上記第
1の電源を降圧して上記電磁コイルを付勢する必要がな
くなり、上記直列抵抗による電力消費を節約できる効果
を有するものである。
By the way, in the above explanation, the case where this invention is used for an electromagnetic brake provided on the hoisting side of an elevator has been described, but it can also be used for other electromagnetic devices1. After energizing the electromagnetic coil with the first 'Ff source having a high DC voltage and operating all the operating parts by the magnetic force of this electromagnetic coil, switching to the second power supply having a DC voltage lower than the first power supply. Since the operating state is maintained by switching the electromagnetic coil using a series resistor, there is no need to step down the voltage of the first power source using a series resistor to energize the electromagnetic coil, which has the effect of saving power consumption due to the series resistor. It is.

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

第1図はエレベータの巻上様の正面図、第2図はエレベ
ータの巻上様に適用された従来の電磁石装置の制御回路
図、第3図はこの発明の一実施例し1中、(9)は作動
部、 a21は電磁コイル、α3はブレーキ接点(切換
手段)、(7)は第1の電源、G1)は第2の電源、 
(41)は時限リレー(時計手段)である。 代理人 葛野信− 元 1 日
FIG. 1 is a front view of an elevator hoisting system, FIG. 2 is a control circuit diagram of a conventional electromagnetic device applied to an elevator hoisting system, and FIG. 3 is an embodiment of the present invention. 9) is the actuating part, a21 is the electromagnetic coil, α3 is the brake contact (switching means), (7) is the first power source, G1) is the second power source,
(41) is a time relay (clock means). Agent Makoto Kuzuno - former 1st

Claims (1)

【特許請求の範囲】 +1)  直流電源で付勢される電磁コイル、この電磁
コイルの付勢を介して作動する作動部、上記電磁コイル
を付勢して上記作動部を非作動状態から作動状態へ移行
させる第1の電源、この第1の電源よジも低い電圧で上
記電磁コイルを付勢して上記作動部を作動状態に保持す
る第2の電源、上記電磁コイルの付勢状態を上記第1の
電源から上記第2の電源へ切り換える切換手段を備えた
電磁石装置。 (2)  作動部は1作動によってブレーキの制動状態
ヲ解りものとしたことを特徴とする特許請求の範囲第1
項記載の電磁石装置。 (3)  第1の電源と第2の電源は同極性に接続され
、かつ、第2の電源は逆流阻止機能を有するものとした
ことを特徴とする特許請求の範囲第1項記載の電磁石装
置。 (4)  切換手段は9作動部に連動するものとしたこ
とを特徴とする特許請求の範囲第1項記載の電磁石装置
。 (5)  切換手段は、第1の電源による付勢から所定
時間の経過を介して切り換える時計手段としたことを特
徴とする特許請求の範囲第1項記載の電磁石装置。
[Scope of Claims] +1) An electromagnetic coil energized by a DC power supply, an actuating section that operates through the energization of the electromagnetic coil, and energizing the electromagnetic coil to change the operating section from a non-operating state to an operating state. a first power source that energizes the electromagnetic coil at a voltage lower than that of the first power source to maintain the actuating section in the operating state; An electromagnetic device comprising a switching means for switching from the first power source to the second power source. (2) Claim 1, characterized in that the actuating section is capable of determining the braking state of the brake by one operation.
Electromagnetic device as described in section. (3) The electromagnet device according to claim 1, wherein the first power source and the second power source are connected with the same polarity, and the second power source has a backflow prevention function. . (4) The electromagnet device according to claim 1, wherein the switching means is interlocked with nine actuating parts. (5) The electromagnetic device according to claim 1, wherein the switching means is a clock means that switches the switching after a predetermined period of time has elapsed since energization by the first power source.
JP57159874A 1982-09-14 1982-09-14 Electromagnet device Pending JPS5948903A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57159874A JPS5948903A (en) 1982-09-14 1982-09-14 Electromagnet device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57159874A JPS5948903A (en) 1982-09-14 1982-09-14 Electromagnet device

Publications (1)

Publication Number Publication Date
JPS5948903A true JPS5948903A (en) 1984-03-21

Family

ID=15703087

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57159874A Pending JPS5948903A (en) 1982-09-14 1982-09-14 Electromagnet device

Country Status (1)

Country Link
JP (1) JPS5948903A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4974703A (en) * 1988-06-27 1990-12-04 Mitsubishi Denki Kabushikia Kaisha Elevator control apparatus
EP0843324A1 (en) * 1996-11-18 1998-05-20 Schneider Electric Sa A power supply circuit for an electromagnet
EP1437554A1 (en) * 2001-09-26 2004-07-14 Daikin Industries, Ltd. Solenoid valve control device and air conditioner provided with solenoid valve control device

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4974703A (en) * 1988-06-27 1990-12-04 Mitsubishi Denki Kabushikia Kaisha Elevator control apparatus
EP0843324A1 (en) * 1996-11-18 1998-05-20 Schneider Electric Sa A power supply circuit for an electromagnet
FR2756091A1 (en) * 1996-11-18 1998-05-22 Schneider Electric Sa FEEDING CIRCUIT OF A COIL FOR ELECTRO-MAGNET
EP1437554A1 (en) * 2001-09-26 2004-07-14 Daikin Industries, Ltd. Solenoid valve control device and air conditioner provided with solenoid valve control device
EP1437554A4 (en) * 2001-09-26 2007-03-28 Daikin Ind Ltd Solenoid valve control device and air conditioner provided with solenoid valve control device

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