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JPS5821809B2 - Demagnetizing device - Google Patents
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JPS5821809B2 - Demagnetizing device - Google Patents

Demagnetizing device

Info

Publication number
JPS5821809B2
JPS5821809B2 JP1333380A JP1333380A JPS5821809B2 JP S5821809 B2 JPS5821809 B2 JP S5821809B2 JP 1333380 A JP1333380 A JP 1333380A JP 1333380 A JP1333380 A JP 1333380A JP S5821809 B2 JPS5821809 B2 JP S5821809B2
Authority
JP
Japan
Prior art keywords
circuit
magnetic
demagnetizing
current
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.)
Expired
Application number
JP1333380A
Other languages
Japanese (ja)
Other versions
JPS56110209A (en
Inventor
三村桂
津川和夫
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 JP1333380A priority Critical patent/JPS5821809B2/en
Publication of JPS56110209A publication Critical patent/JPS56110209A/en
Publication of JPS5821809B2 publication Critical patent/JPS5821809B2/en
Expired legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F13/00Apparatus or processes for magnetising or demagnetising
    • H01F13/006Methods and devices for demagnetising of magnetic bodies, e.g. workpieces, sheet material

Landscapes

  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Measuring Magnetic Variables (AREA)
  • Control Of Linear Motors (AREA)

Description

【発明の詳細な説明】 本発明は既に着磁(帯磁)された磁気量を減磁する減磁
装置の改良に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an improvement in a demagnetizing device that demagnetizes a magnetic quantity that has already been magnetized.

この種の装置は誘導円板形過電流継電器、誘導円板形電
圧継電器あるいは誘導円板形積算電力計等の制動に用い
られる永久磁石又は一般に可動線輪型電圧計あるいは電
流計の永久磁石の磁化を一定値に設定する時などにしば
しは用いられる装置ンである。
This type of device is a permanent magnet used for braking of an induction disk overcurrent relay, an induction disk voltage relay, an induction disk integrated wattmeter, etc., or a permanent magnet of a movable ring voltmeter or ammeter. This is a device that is often used when setting magnetization to a constant value.

従来この種の減磁装置として第1図あるいは第2図に示
す如き減磁装置が提案されている。
Conventionally, a demagnetizing device as shown in FIG. 1 or 2 has been proposed as this type of demagnetizing device.

第1図の減磁装置は、直流電源電圧EDが印加されて磁
束φ1が発生させるソレノイド1a、1bと磁I気回路
を構成する鉄心2とを備えた構成となっている。
The demagnetizing device shown in FIG. 1 includes solenoids 1a and 1b to which a DC power supply voltage ED is applied to generate a magnetic flux φ1, and an iron core 2 forming a magnetic I-magnetic circuit.

又第2図の減磁装置は、交流電源電圧EAが印加されて
交番磁束φ1.φ3を発生させるソレノイド1aから成
っている。
Further, the demagnetizing device shown in FIG. 2 generates an alternating magnetic flux φ1. It consists of a solenoid 1a that generates φ3.

3は永久磁石で、この永久磁石は所定の磁化以上に着磁
されており、2減磁装置により最終的に目的とする磁化
量だけ着磁される。
Reference numeral 3 denotes a permanent magnet, which is magnetized to a predetermined magnetization level or higher, and is finally magnetized to a desired amount of magnetization by a demagnetizing device 2.

次にこれらの減磁装置の動作を説明する。Next, the operation of these demagnetizing devices will be explained.

第1図に於て直流電源電圧EDがソレノイド1a、1b
に印加されるとソレノイド1a、1bの合成直流デ抵抗
で制御された電流■。
In Figure 1, the DC power supply voltage ED is
When applied to solenoid 1a, 1b, the combined DC current is controlled by resistance.

が流れる。ソレノイド1a、1bの合成巻数をTいまた
磁気回路の合成磁気抵抗をRmとすると磁束φ1が次式
(1)により与えられる。
flows. If the combined number of turns of the solenoids 1a and 1b is T, and the combined magnetic resistance of the magnetic circuit is Rm, then the magnetic flux φ1 is given by the following equation (1).

又鉄心の端面は磁極N、Sとなる電磁界が生じることは
周知である。
Furthermore, it is well known that an electromagnetic field that becomes magnetic poles N and S is generated at the end face of the iron core.

今、減磁を必要とする永久磁石3を永久磁石の持つ磁極
を電磁界の磁極と反対にして電磁界に近づけると永久磁
石は減磁される。
Now, when the permanent magnet 3 that requires demagnetization is brought close to the electromagnetic field with the magnetic pole of the permanent magnet opposite to the magnetic pole of the electromagnetic field, the permanent magnet will be demagnetized.

第2図に於て交流電源電圧EAがソレノイド1aに印加
されると、ソレノイド1aのインピーダンスで制限され
た電流れが流れる。
In FIG. 2, when AC power supply voltage EA is applied to solenoid 1a, a current flow limited by the impedance of solenoid 1a flows.

ソレノイド1aの巻数をTa、また磁気回路の磁気抵抗
をRaとすると交番磁束φ3が次式(2)により与えら
れ交番電磁界がソレノイド1aの端面に生じる。
When the number of turns of the solenoid 1a is Ta, and the magnetic resistance of the magnetic circuit is Ra, an alternating magnetic flux φ3 is given by the following equation (2), and an alternating electromagnetic field is generated at the end face of the solenoid 1a.

前述と同様に減磁を必要とする永久磁石3をソレノイド
1aに第2図に示す如く垂直に近づけると、交番電磁界
が永久磁石の磁性と反対になっているとき永久磁石は減
磁される。
Similarly to the above, when the permanent magnet 3 that requires demagnetization is brought vertically close to the solenoid 1a as shown in Figure 2, the permanent magnet will be demagnetized when the alternating electromagnetic field is opposite to the magnetism of the permanent magnet. .

しかしながら、従来の減磁装置は以上のように構成され
ているので、永久磁石を所望の磁界の強さに減磁する必
要があっても、減磁装置に近づける距離等の管理が困難
であり、又減磁された永久磁石の強さをあらためて計測
せねば所望の磁界の強さになっているかどうかを知るこ
とができないなどの欠点があった。
However, since conventional demagnetizing devices are configured as described above, even if it is necessary to demagnetize the permanent magnet to a desired magnetic field strength, it is difficult to manage the distance to bring the permanent magnet close to the demagnetizing device. Another disadvantage is that it is impossible to know whether the desired magnetic field strength is achieved unless the strength of the demagnetized permanent magnet is measured again.

この発明は上記のような従来のものの欠点を除去するた
めになされたもので、磁性体の着磁の程度を磁気感応素
子を用いて検出し、これを基準値。
This invention was made in order to eliminate the above-mentioned drawbacks of the conventional ones.The degree of magnetization of a magnetic material is detected using a magnetic sensing element, and this is set as a reference value.

と比較し、前記磁性体の磁化の強さを所望する任意の値
に設定できる減磁装置を提供することを目的としている
It is an object of the present invention to provide a demagnetizing device that can set the magnetization strength of the magnetic material to any desired value.

以下、この発明の一実施例を図について説明する。An embodiment of the present invention will be described below with reference to the drawings.

尚以下、第1図及び第2図と同一符号は同−或いは相当
部分を示すにつき、符号の説明は適宜省略する。
Hereinafter, the same reference numerals as in FIGS. 1 and 2 indicate the same or corresponding parts, and the explanation of the reference numerals will be omitted as appropriate.

第3図において、3は所望の値に減磁される永久磁石、
4は電流制御回路、4aは電流制御回路。
In Fig. 3, 3 is a permanent magnet that is demagnetized to a desired value;
4 is a current control circuit; 4a is a current control circuit;

内のスライダック、4a1はスライダック4aの可動部
、4bはこの可動部4a1を駆動するモータ、5はソレ
ノイド1aへの給電を停止する電流遮断回路、5aは電
流遮断回路5の電磁開閉器のb接点、5bは電流遮断回
路5の電磁開閉器の付。
4a1 is the movable part of the slider 4a, 4b is the motor that drives this movable part 4a1, 5 is a current cutoff circuit that stops power supply to the solenoid 1a, and 5a is the b contact of the electromagnetic switch of the current cutoff circuit 5. , 5b is the attachment of the electromagnetic switch of the current interrupting circuit 5.

勢用コイル、6は磁束検出回路、6aは磁気感応手段で
あるホール素子、6bは変換回路、7は比較回路である
6 is a magnetic flux detection circuit, 6a is a Hall element which is a magnetic sensing means, 6b is a conversion circuit, and 7 is a comparison circuit.

8は電流制御回路の起動スイッチである。8 is a start switch for the current control circuit.

次にこの減磁装置の動作を第4図及び第5図a〜eに示
す各部の波形図を参照にして説明する。
Next, the operation of this demagnetizing device will be explained with reference to waveform diagrams of various parts shown in FIGS. 4 and 5 a to 5 e.

尚第5図a = eにおいて横軸に時間tを、縦軸は電
圧、電流、磁気量などの物理量をそれぞれ示している。
In FIG. 5 a = e, the horizontal axis represents time t, and the vertical axis represents physical quantities such as voltage, current, and magnetic quantity.

第3図の電流制御回路4に第5図aに示す交流電源電圧
を印加し、次に第3図の電流制御回路の起動スイッチ8
が閉じられると電流制御回路4内のモータ4bが動きだ
し、機械的に接続されたスライダック4aの可動部4a
lも同時に動き出す。
The AC power supply voltage shown in FIG. 5a is applied to the current control circuit 4 shown in FIG. 3, and then the starting switch 8 of the current control circuit shown in FIG.
When the motor 4b in the current control circuit 4 is closed, the motor 4b in the current control circuit 4 starts moving, and the movable part 4a of the mechanically connected slide duck 4a
l also starts moving at the same time.

このとき、スライダック4aの可動部4alはほぼ一定
の速度で駆動されていくので、電流遮断回路5の出力は
第5図すの如く零から除徐に大きくなっていく。
At this time, since the movable part 4al of the slide duck 4a is driven at a substantially constant speed, the output of the current cutoff circuit 5 gradually increases from zero as shown in FIG.

今、第3図のソレノイド1aのインピーダンスが理想的
なコイルで抵抗器がないものとすると、ソレノイド1a
内を流れる電流ハは第5図すより90°遅れることは周
知である。
Now, assuming that the impedance of solenoid 1a in Fig. 3 is an ideal coil and there is no resistor, solenoid 1a
It is well known that the current flowing through the capacitor lags 90° behind that shown in FIG.

従ってソレノイドが発生させる交番磁束φ3は第5図C
となる。
Therefore, the alternating magnetic flux φ3 generated by the solenoid is shown in Figure 5C.
becomes.

ところで、第3図の永久磁石3の空隙内の磁束Bに挿入
されたホール素子6aは第4図に示すように、1面に定
電流I。
By the way, as shown in FIG. 4, the Hall element 6a inserted into the magnetic flux B in the air gap of the permanent magnet 3 shown in FIG. 3 receives a constant current I on one surface.

を流すと、残りの一面より次式(3)の電圧を発生させ
る。
When , the voltage expressed by the following equation (3) is generated from the remaining surface.

■H二K・Io−B ・・・・・・・・・
(3)ここにKはホール素子によって定まる定数で実用
上積感度としてm■/mA−KGで表わされる。
■H2K・Io-B ・・・・・・・・・
(3) Here, K is a constant determined by the Hall element and is expressed as the practical product sensitivity in m/mA-KG.

(Gはガウス) ホール素子6aで発生された電圧は変換回路6bで適当
な出力電圧に変換され第5図dのE。
(G is Gauss) The voltage generated by the Hall element 6a is converted into an appropriate output voltage by the conversion circuit 6b, as shown in E of FIG. 5d.

となって比較回路7のin put端子に印加、される
is applied to the input terminal of the comparator circuit 7.

一方比較回路7の他の端子には、第3図に示されるよう
に直流電圧を可変抵抗器Rpによって分圧された基準電
圧E8が印加されている。
On the other hand, a reference voltage E8, which is a DC voltage divided by a variable resistor Rp, is applied to the other terminal of the comparator circuit 7, as shown in FIG.

従って電流制御回路4が起動した直前では第5図dの如
く磁束検出回路の出力電圧E。
Therefore, immediately before the current control circuit 4 is activated, the output voltage E of the magnetic flux detection circuit is as shown in FIG. 5d.

〉基準電圧E11.であるが電流制御回路4によってソ
レノイド1aに発生される磁束φ3が大きくなると、永
久磁石3は減磁され磁束φ2は減少し磁束検出回路6の
出力電圧が低下して基準電圧E□の方が大きくなる。
>Reference voltage E11. However, when the magnetic flux φ3 generated in the solenoid 1a by the current control circuit 4 increases, the permanent magnet 3 is demagnetized, the magnetic flux φ2 decreases, the output voltage of the magnetic flux detection circuit 6 decreases, and the reference voltage E□ becomes higher. growing.

このとき比較回路7の出力out putは今まで零で
あったが、第5図eに示す如< E(V)を出力する。
At this time, the output of the comparator circuit 7 has been zero until now, but it outputs <E(V) as shown in FIG. 5e.

この電圧により電流遮断回路5の電磁開閉器のコイル5
bは付勢されb接点5aを開放する。
This voltage causes the coil 5 of the electromagnetic switch of the current cutoff circuit 5 to
b is energized and opens the b contact 5a.

このためこの時点以後は、第5図すに示すようにソレノ
イドコイル1aの入力電圧は0〔■〕となり、磁束φ3
も零となり、永久磁石3の減磁を完了する。
Therefore, after this point, the input voltage of the solenoid coil 1a becomes 0 [■] as shown in Fig. 5, and the magnetic flux φ3
also becomes zero, and the demagnetization of the permanent magnet 3 is completed.

次に第6図に従って磁束検出回路6の具体的な詳細を、
又第7図に従って比較回路7の具体的な詳細を説明する
Next, specific details of the magnetic flux detection circuit 6 are explained according to FIG.
Further, specific details of the comparator circuit 7 will be explained according to FIG.

第6図に示される磁束検出回路6はホール素子6aと変
換回路6bとからなり、この変換回路6bは可変抵抗6
b1、固定抵抗6b2〜6b5、演算増巾器6b6等で
構成される。
The magnetic flux detection circuit 6 shown in FIG. 6 consists of a Hall element 6a and a conversion circuit 6b, and this conversion circuit 6b has a variable resistance 6.
b1, fixed resistors 6b2 to 6b5, an operational amplifier 6b6, and the like.

P、Nは直流のプラス、マイナス電源電圧端子を示す。P and N indicate DC plus and minus power supply voltage terminals.

上記の構成でホール素子6aに可変抵抗6blで制限さ
れた電流I。
In the above configuration, the current I is limited by the variable resistor 6bl in the Hall element 6a.

が通電され、磁束Bの中にホール素子6aを置くと前述
(3)式によりホール素子6aは電圧■□を発生させる
When energized and the Hall element 6a is placed in the magnetic flux B, the Hall element 6a generates a voltage ■□ according to the above-mentioned equation (3).

演算増巾器6b6と抵抗6b2〜6b5で作られた差動
増巾回路(変換回路6b)はホール素子6aの電圧VH
を下記(4)式により適当な電圧Voutに増巾するこ
とができる。
A differential amplification circuit (conversion circuit 6b) made of an operational amplifier 6b6 and resistors 6b2 to 6b5 converts the voltage VH of the Hall element 6a.
can be amplified to an appropriate voltage Vout using the following equation (4).

A Voul= −−VH”−甲°(4) B 但し、RA=抵抗6b3の値=抵抗6b5の値RB−抵
抗6b2の値−抵抗6b4の値 比較回路7については第7図に示すようにトランジスタ
7T1〜7T3、固定抵抗7R1〜7R4で構成されて
いる。
A Voul=--VH"-K°(4) B However, RA=value of resistor 6b3=value of resistor 6b5 RB-value of resistor 6b2-value of resistor 6b4 Regarding the comparison circuit 7, as shown in FIG. It is composed of transistors 7T1 to 7T3 and fixed resistors 7R1 to 7R4.

上記の構成で比較回路7の基準電圧入力端子REFに電
圧EfL1比較電圧入力端子in putにE。
With the above configuration, a voltage EfL1 is applied to the reference voltage input terminal REF of the comparison circuit 7, and E is applied to the comparison voltage input terminal input.

が印加された場合、E−PL<E。であるとトランジス
タ7T2はオンとなりトランジスタ7T1はカットオフ
されトランジスタ7T1のコレクタ電圧はPとなりこの
ためトランジスタ7T3はオフとなり出力電圧Vout
はOとなる。
is applied, E-PL<E. Then, the transistor 7T2 is turned on, the transistor 7T1 is cut off, and the collector voltage of the transistor 7T1 becomes P. Therefore, the transistor 7T3 is turned off, and the output voltage Vout
becomes O.

次にER,〉Eoとなるとトランジスタ7T1がオンと
なりトランジスタ7T2はカットオフされる。
Next, when ER,>Eo, the transistor 7T1 is turned on and the transistor 7T2 is cut off.

このトランジスタ7T1がオンすることによりトランジ
スタ7T1のコレクタ電圧が下がり、トランジスタ7T
3より点線の18が流れることができトランジスタ7T
3はオンとなり出力端子VoutはほぼP電圧となる。
By turning on this transistor 7T1, the collector voltage of the transistor 7T1 decreases, and the transistor 7T
Transistor 7T allows the dotted line 18 to flow from 3.
3 is turned on, and the output terminal Vout becomes approximately P voltage.

以上のように構成することにより磁束検出回路6、比較
回路7は簡単に得ることができる。
By configuring as described above, the magnetic flux detection circuit 6 and the comparison circuit 7 can be easily obtained.

尚、上記実施例ではソレノイド1aを交流励磁している
ので、永久磁石3を減磁するにあたり、その極性につい
て考慮する必要がなく、作業上の利点もある。
In the above embodiment, since the solenoid 1a is excited with alternating current, there is no need to consider the polarity when demagnetizing the permanent magnet 3, which is advantageous in terms of work.

なお上記実施例では電流制御回路4にスライダック4a
とモータ4bとを設けたものを示したが電流制御回路4
、スライダック4aの代わりに摺動抵抗を設けてもよい
In the above embodiment, the current control circuit 4 includes a slider 4a.
The current control circuit 4 is shown as having a motor 4b and a motor 4b.
, a sliding resistance may be provided in place of the sliding duck 4a.

又電流制御回路4と電流遮断回路5とを一体の回路とし
てもよい。
Further, the current control circuit 4 and the current cutoff circuit 5 may be formed as an integrated circuit.

更に第3図のソレノイド1aは空心であるが第1図に示
す如き鉄心2にソレノイドia、ibを巻回する構成と
してもよい。
Furthermore, although the solenoid 1a shown in FIG. 3 has an air core, the solenoid ia and ib may be wound around an iron core 2 as shown in FIG.

次にこの発明の他の実施例を第8図、第9図について説
明する。
Next, another embodiment of the present invention will be described with reference to FIGS. 8 and 9.

この実施例では、交流電源Eaからの交流を直流変換回
路9を介して一旦直流に変換し、これを電流制御回路4
に供給する構成である。
In this embodiment, alternating current from an alternating current power source Ea is once converted to direct current via a direct current conversion circuit 9, and then converted into direct current by a current control circuit 4.
It is configured to supply

その他の部分については、前述の実施例とほぼ同様な構
成としている。
The other parts have almost the same configuration as the previous embodiment.

このような構成のものの動作を第9図に従って説明する
と、各部の波形は第9図の如くなる。
The operation of the device having such a configuration will be explained with reference to FIG. 9. The waveforms of each part will be as shown in FIG.

すなわち、直流変換回路9に第9図aの交流電圧が印加
されると直流変換回路9の出力は同図すの波形となる。
That is, when the AC voltage shown in FIG. 9a is applied to the DC conversion circuit 9, the output of the DC conversion circuit 9 has the waveform shown in FIG.

次に第8図の電流制御回路の起動スイッチ8が閉じられ
制御電圧が電流制御回路4のモータ4bに印加されモー
タ4bが動き、モータに連動して可変抵抗4aの可動部
4a1が可変抵抗のA点からB点まで動く場合、可変抵
抗4aの値が無限大から零オーム間変化する。
Next, the starting switch 8 of the current control circuit shown in FIG. When moving from point A to point B, the value of variable resistor 4a changes from infinity to zero ohms.

このときソレノイド1aの直流抵抗1がSオームとする
とソレノイド1aに流れる電流I、は次の式で与えられ
る電流値の範囲となる。
At this time, if the DC resistance 1 of the solenoid 1a is S ohm, the current I flowing through the solenoid 1a falls within the range of current values given by the following equation.

D ID1= −=0 0 D ID2−− ここに、■ 1は最小電流、ID2は最大電流である。D ID1=-=0 0 D ID2-- Here, (1) is the minimum current, and ID2 is the maximum current.

今、ソレノイド1aに第8図に示す方向に電流が流れる
と第8図に示す如く磁束φ3が発生することは前述の実
施例と同様である。
Now, when a current flows through the solenoid 1a in the direction shown in FIG. 8, a magnetic flux φ3 is generated as shown in FIG. 8, as in the previous embodiment.

第8図の)磁束φ3の磁極に相反する磁極となるよう減
磁しようとする方向に永久磁石3を置き、永久磁石3の
空隙の磁束φ2内にホール素子6aを挿入すればよい。
The permanent magnet 3 is placed in the direction in which demagnetization is desired so that the magnetic pole is opposite to the magnetic pole of the magnetic flux φ3 (in FIG. 8), and the Hall element 6a is inserted into the magnetic flux φ2 in the gap of the permanent magnet 3.

なおこの実施例では交流電源電圧Eaを用い直1流変換
回路で直流電圧EDを作っているが、交流電源電圧の代
わりに直流電源電圧を用い直流変換回路を省略してもよ
い。
In this embodiment, the AC power supply voltage Ea is used to generate the DC voltage ED using a direct-to-current conversion circuit, but the DC power supply voltage may be used instead of the AC power supply voltage and the DC conversion circuit may be omitted.

又電流制御回路と電流遮断回路を一体の回路としてもよ
い。
Further, the current control circuit and the current cutoff circuit may be integrated into one circuit.

更に第3図のソレノイド1aは空心であるが第1図に示
す如きノ鉄心2にソレノイド1a、1bを巻回する構成
としてもよい。
Furthermore, although the solenoid 1a in FIG. 3 has an air core, the solenoids 1a and 1b may be wound around an iron core 2 as shown in FIG.

その場合には、交流励磁方式にくらべ鉄心2に種々の損
失が発生しないという利点がある。
In that case, there is an advantage that various losses do not occur in the iron core 2 compared to the AC excitation method.

以上のように、この発明によれば減磁を必要とする既着
磁の磁性体の磁束を磁気感応手段を用いて検出し、減磁
する磁束の強さを徐々に零から大きくするようにし、更
に比較回路で磁性体の磁束を基準値と比較し自動的に減
磁する磁束を遮断するように構成したので磁性体の磁束
の強さを一定値に簡単にできまた精度の高いものが得ら
れる効果がある。
As described above, according to the present invention, the magnetic flux of a magnetized magnetic body that requires demagnetization is detected using a magnetically sensitive means, and the strength of the magnetic flux to be demagnetized is gradually increased from zero. Furthermore, the comparator circuit is configured to compare the magnetic flux of the magnetic material with a reference value and automatically cut off the demagnetizing magnetic flux, making it possible to easily maintain the strength of the magnetic flux of the magnetic material at a constant value and to achieve high accuracy. There are benefits to be gained.

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

第1図、第2図は従来の減磁装置のブ爾ツク図、第3図
は本発明に係る減磁装置の一実施例を示すブロック図、
第4図はホール素子の原理を示す図、第5図a −eは
第3図に示したものの各部の動作波形図、第6図は磁束
検出回路の詳細を示す回路図、第7図は比較回路の詳細
を示す回路図、第8図は本発明に係る減磁装置の他の実
施例を示すブロック図、第9図a −fは第8図に示し
たものの各部の動作波形図である。 図において、EAは交流電源、Eは直流電源、1は励磁
手段、3は永久磁石、4は直流制御回路、5は電流遮断
回路、6は磁束検出回路、γは比較回路、8は起動用ス
イッチである。 なお図中同一符号は同−或いは相当部分を示す。
1 and 2 are block diagrams of a conventional demagnetizing device, and FIG. 3 is a block diagram showing an embodiment of a demagnetizing device according to the present invention.
Figure 4 is a diagram showing the principle of the Hall element, Figures 5a-e are operational waveform diagrams of each part shown in Figure 3, Figure 6 is a circuit diagram showing details of the magnetic flux detection circuit, and Figure 7 is a diagram showing the details of the magnetic flux detection circuit. FIG. 8 is a block diagram showing another embodiment of the demagnetizing device according to the present invention, and FIGS. 9 a - f are operation waveform diagrams of each part of the circuit shown in FIG. be. In the figure, EA is an AC power supply, E is a DC power supply, 1 is an excitation means, 3 is a permanent magnet, 4 is a DC control circuit, 5 is a current cutoff circuit, 6 is a magnetic flux detection circuit, γ is a comparison circuit, and 8 is for starting. It's a switch. Note that the same reference numerals in the figures indicate the same or equivalent parts.

Claims (1)

【特許請求の範囲】 1 予め磁化されている磁性体の着磁量を減磁して、所
定値に着磁する装置において、電源、この電源により励
磁され、上記磁性体の磁化力を減磁する磁界を発生する
励磁手段、この励磁手段と上記電源との間に接続され、
上記励磁手段への給電量を制御して減磁する磁界の強さ
を零から徐々に増加する電流制御回路、上記磁性体の着
磁量に応動するように配設された磁気感応手段を有し、
この磁気感応手段の出力を検出することにより上記磁性
体の着磁量を検出する検出回路、この検出回路の検出値
を基準値と比較する比較回路、およびこの比較回路の比
較結果に応動じて上記励磁手段への給電を停止する電流
遮断回路を備えた減磁装置。 2 電流制御回路はスライダックと、始動信号により前
記スライダックの可動部を駆動するモータとからなるこ
とを特徴とする特許請求の範囲第1項記載の減磁装置。
[Scope of Claims] 1. A device for demagnetizing a pre-magnetized magnetic body to a predetermined value by demagnetizing it to a predetermined value; an excitation means for generating a magnetic field, connected between the excitation means and the power supply,
It has a current control circuit that gradually increases the strength of the demagnetizing magnetic field from zero by controlling the amount of power supplied to the excitation means, and a magnetic sensing means arranged to respond to the amount of magnetization of the magnetic body. death,
A detection circuit that detects the amount of magnetization of the magnetic body by detecting the output of this magnetic sensing means, a comparison circuit that compares the detected value of this detection circuit with a reference value, and a detection circuit that responds to the comparison result of this comparison circuit. A demagnetizing device comprising a current cutoff circuit for stopping power supply to the excitation means. 2. The demagnetizing device according to claim 1, wherein the current control circuit comprises a slider and a motor that drives the movable part of the slider in response to a start signal.
JP1333380A 1980-02-05 1980-02-05 Demagnetizing device Expired JPS5821809B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1333380A JPS5821809B2 (en) 1980-02-05 1980-02-05 Demagnetizing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1333380A JPS5821809B2 (en) 1980-02-05 1980-02-05 Demagnetizing device

Related Child Applications (1)

Application Number Title Priority Date Filing Date
JP534083A Division JPS5849009B2 (en) 1983-01-18 1983-01-18 Demagnetizing device

Publications (2)

Publication Number Publication Date
JPS56110209A JPS56110209A (en) 1981-09-01
JPS5821809B2 true JPS5821809B2 (en) 1983-05-04

Family

ID=11830199

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1333380A Expired JPS5821809B2 (en) 1980-02-05 1980-02-05 Demagnetizing device

Country Status (1)

Country Link
JP (1) JPS5821809B2 (en)

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US10316501B2 (en) * 2016-07-29 2019-06-11 Hydrotek Corporation Control method and circuit of a controller for a battery operated water faucet

Also Published As

Publication number Publication date
JPS56110209A (en) 1981-09-01

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