JPS6058565B2 - Magnetization method of asymmetric multipolar magnet disk - Google Patents

Magnetization method of asymmetric multipolar magnet disk

Info

Publication number
JPS6058565B2
JPS6058565B2 JP8244878A JP8244878A JPS6058565B2 JP S6058565 B2 JPS6058565 B2 JP S6058565B2 JP 8244878 A JP8244878 A JP 8244878A JP 8244878 A JP8244878 A JP 8244878A JP S6058565 B2 JPS6058565 B2 JP S6058565B2
Authority
JP
Japan
Prior art keywords
asymmetric
pole
multipolar magnet
magnet disk
windings
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
JP8244878A
Other languages
Japanese (ja)
Other versions
JPS559456A (en
Inventor
勝啓 太田
清 下澤
多賀雄 杉崎
実 日暮
覚 北原
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.)
TDK Corp
Original Assignee
TDK 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 TDK Corp filed Critical TDK Corp
Priority to JP8244878A priority Critical patent/JPS6058565B2/en
Publication of JPS559456A publication Critical patent/JPS559456A/en
Publication of JPS6058565B2 publication Critical patent/JPS6058565B2/en
Expired legal-status Critical Current

Links

Description

【発明の詳細な説明】 本発明は、非対称多極磁界を発生するための非対称多
極マグネット円板の着磁方法に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method of magnetizing an asymmetric multipolar magnet disk for generating an asymmetric multipolar magnetic field.

回転角度、回転速度等の検出用には、多極マグネット
円板が用いられることが多いが、その多極マグネット円
板に着磁された磁極の強さは皆同一であるのが普通であ
る。従つて、そのような多極マグネット円板では、第1
図の如き、交番対称磁界が回転に伴つて生じる。ところ
で、用途によつては、第2図に示すように交番非対称磁
界を回転に伴つて発生することが要求される場合があり
、このためには磁極の表面磁束密度を位置に応じて大き
くあるいは小さく変えなければならない。従つて、通常
の多極マグネット円板の着磁方法をそのまま採用するこ
とはできない。 本発明は、上記の点に鑑み、1囲の着
磁操作により位置に応じて磁極に強弱をつけることが可
能な非対称多極マグネット円板の着磁方法を提供しよう
とするものである。 以下、本発明に係る非対称多極マ
グネット円板の着磁方法の実施例を図面に従つて説明す
る。
A multipolar magnet disk is often used to detect rotation angle, rotation speed, etc., but the strength of the magnetic poles magnetized on the multipolar magnet disk is usually the same. . Therefore, in such a multipolar magnetic disk, the first
As shown in the figure, an alternating symmetrical magnetic field is generated with rotation. By the way, depending on the application, it may be required to generate an alternating asymmetrical magnetic field with rotation as shown in Figure 2, and for this purpose, the surface magnetic flux density of the magnetic poles may be increased or decreased depending on the position. I have to make small changes. Therefore, the usual method of magnetizing a multipolar magnet disk cannot be used as is. In view of the above-mentioned points, the present invention provides a method for magnetizing an asymmetric multipolar magnet disk, which allows magnetic poles to be made stronger or weaker depending on the position by magnetizing operations in one circle. DESCRIPTION OF THE PREFERRED EMBODIMENTS Examples of the method of magnetizing an asymmetric multipolar magnet disk according to the present invention will be described below with reference to the drawings.

第3図において、着磁用ヨーク1は、円筒状であつて
、内周面に等間隔で極部2A乃至2Fが形成されている
。そして、極部2A、2C、2Eの両側には深いスロッ
ト3が形成され、極部2B、2D、2Fの両側には浅い
スロット4が形成される。各極部2A乃至2Fの両側ス
ロット3、4は夫々の巻線5A乃至5Fが収納され、各
巻線は順次直列接続される。ここで、巻線5A、5C、
5Eと巻線5B、5D、5Fとは巻線方向が逆向きにな
つている。上記の如き着磁用ヨーク1内に着磁前の磁性
体円板6を設置し、極部2A乃至2Fを磁性体円板6の
周面に対向させた状態で直流電源7を巻線引出端8A,
8Bに接続すれば、各巻線5A乃至5Fを数100A程
度の電流が瞬間的に流れ着磁が実行される。
In FIG. 3, the magnetizing yoke 1 has a cylindrical shape, and pole portions 2A to 2F are formed at equal intervals on the inner peripheral surface. Further, deep slots 3 are formed on both sides of the pole parts 2A, 2C, and 2E, and shallow slots 4 are formed on both sides of the pole parts 2B, 2D, and 2F. The slots 3 and 4 on both sides of each of the pole parts 2A to 2F accommodate respective windings 5A to 5F, and the windings are connected in series in sequence. Here, windings 5A, 5C,
The winding directions of 5E and windings 5B, 5D, and 5F are opposite to each other. The magnetic disk 6 before magnetization is installed in the magnetization yoke 1 as described above, and the DC power source 7 is drawn out with the windings with the pole parts 2A to 2F facing the circumferential surface of the magnetic disk 6. End 8A,
8B, a current of about several hundred amperes instantaneously flows through each winding 5A to 5F, and magnetization is executed.

このとき、巻線5A乃至5Fは直列接続されているので
、各巻線に流れる電流は同じであるが、スロットの深さ
、すなわち巻線の深さ方向位置が極部によつて異なつて
いるから、巻線位置の浅い極部2B,2D,2Fに強い
磁界が発生され、巻線位置の深い極部2A,2C,2E
に比較的弱い逆向きの磁界が発生される。これは、巻線
位置が深いとそれだけ極部が長くなり、該極部での損失
が増加するためである。従つて、極部2B,2D,2F
に対向する磁性体円板6の周面部分に強い磁極が形成さ
れ、極部2A,2C,2Eに対向する磁性体円板6の周
面部分に比較的弱い逆極性の磁極が形成され、しかして
非対称多極マグネット円板が完成する。上記実施例によ
れば、各極部に設けた巻線の深さを変えることにより、
磁性体円板の周面に強い磁極と弱い磁極とを1回の着磁
操作で同時に形成できる。
At this time, since the windings 5A to 5F are connected in series, the current flowing through each winding is the same, but the depth of the slot, that is, the position in the depth direction of the winding, differs depending on the pole. , a strong magnetic field is generated in the pole parts 2B, 2D, and 2F where the winding position is shallow, and the pole parts 2A, 2C, and 2E where the winding position is deep.
A relatively weak magnetic field in the opposite direction is generated. This is because the deeper the winding position, the longer the pole portion becomes, and the loss at the pole portion increases. Therefore, the pole parts 2B, 2D, 2F
A strong magnetic pole is formed on the circumferential surface portion of the magnetic disk 6 facing the pole portions 2A, 2C, and 2E, and a relatively weak magnetic pole of opposite polarity is formed on the circumferential surface portion of the magnetic disk 6 facing the pole portions 2A, 2C, and 2E. Thus, an asymmetric multipolar magnet disk is completed. According to the above embodiment, by changing the depth of the winding provided at each pole,
A strong magnetic pole and a weak magnetic pole can be simultaneously formed on the circumferential surface of a magnetic disk in one magnetization operation.

なお、着磁用ヨークの極部の数は適宜増減可能であるこ
とは勿論である。
It goes without saying that the number of pole parts of the magnetizing yoke can be increased or decreased as appropriate.

叙上のように、本発明の非対称多極マグネット円板の着
磁方法によれば、1回の着磁操作により位置に応じて磁
極に強弱をつけることが可能である。
As described above, according to the method of magnetizing an asymmetric multipolar magnet disk of the present invention, it is possible to make the magnetic poles stronger or weaker depending on the position by a single magnetization operation.

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

第1図は交番対称磁界の1例を示す説明図、第2図は交
番非対称磁界の1例を示す説明図、第3図は本発明に係
る非対称多極マグネット円板の着磁方法の実施例を示す
断面図である。 1・・・・・・着磁用ヨーク、2A乃至2F・・・・・
・極部、3,4・・・・・・スロット、5A乃至5F・
・・・・・巻線、6・・・・・・磁性体円板、7・・・
・・・直流電源。
FIG. 1 is an explanatory diagram showing an example of an alternating symmetric magnetic field, FIG. 2 is an explanatory diagram showing an example of an alternating asymmetric magnetic field, and FIG. 3 is an implementation of the method for magnetizing an asymmetric multipolar magnet disk according to the present invention. It is a sectional view showing an example. 1... Magnetizing yoke, 2A to 2F...
・Pole part, 3, 4...Slot, 5A to 5F・
... Winding wire, 6 ... Magnetic disk, 7 ...
...DC power supply.

Claims (1)

【特許請求の範囲】[Claims] 1 着磁用ヨークの内周面に形成された複数の極部の周
囲に各極部の位置に応じて異なる深さの巻線を設け、該
巻線を直列に接続し、前記極部に周面が対向するように
磁性体円板を配置した状態で前記巻線に直流電流を流す
ことを特徴とする非対称多極マグネット円板の着磁方法
1. Windings with different depths are provided around the plurality of pole parts formed on the inner circumferential surface of the magnetizing yoke according to the position of each pole part, and the windings are connected in series, and the windings are connected in series to the pole parts. 1. A method of magnetizing an asymmetric multipolar magnet disk, characterized in that a DC current is passed through the windings in a state in which the magnetic disks are arranged so that their circumferential surfaces face each other.
JP8244878A 1978-07-06 1978-07-06 Magnetization method of asymmetric multipolar magnet disk Expired JPS6058565B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8244878A JPS6058565B2 (en) 1978-07-06 1978-07-06 Magnetization method of asymmetric multipolar magnet disk

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8244878A JPS6058565B2 (en) 1978-07-06 1978-07-06 Magnetization method of asymmetric multipolar magnet disk

Publications (2)

Publication Number Publication Date
JPS559456A JPS559456A (en) 1980-01-23
JPS6058565B2 true JPS6058565B2 (en) 1985-12-20

Family

ID=13774797

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8244878A Expired JPS6058565B2 (en) 1978-07-06 1978-07-06 Magnetization method of asymmetric multipolar magnet disk

Country Status (1)

Country Link
JP (1) JPS6058565B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6232852U (en) * 1985-08-13 1987-02-26

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS601820A (en) * 1983-06-17 1985-01-08 Tohoku Metal Ind Ltd Manufacture of cylindrical permanent magnet
JPS61141113A (en) * 1984-12-14 1986-06-28 Hitachi Metals Ltd Manufacture of magnet roll
DE102014105370A1 (en) * 2014-04-15 2015-10-15 Epcos Ag core component

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6232852U (en) * 1985-08-13 1987-02-26

Also Published As

Publication number Publication date
JPS559456A (en) 1980-01-23

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