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JPH0529122B2 - - Google Patents
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JPH0529122B2 - - Google Patents

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Publication number
JPH0529122B2
JPH0529122B2 JP62025585A JP2558587A JPH0529122B2 JP H0529122 B2 JPH0529122 B2 JP H0529122B2 JP 62025585 A JP62025585 A JP 62025585A JP 2558587 A JP2558587 A JP 2558587A JP H0529122 B2 JPH0529122 B2 JP H0529122B2
Authority
JP
Japan
Prior art keywords
magnetic
pole
roller
poles
magnetizing
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 - Lifetime
Application number
JP62025585A
Other languages
Japanese (ja)
Other versions
JPS6464204A (en
Inventor
Naoji Ootsuka
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.)
Canon Inc
Original Assignee
Canon Inc
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 Canon Inc filed Critical Canon Inc
Priority to JP2558587A priority Critical patent/JPS6464204A/en
Priority to US07/049,966 priority patent/US4954800A/en
Publication of JPS6464204A publication Critical patent/JPS6464204A/en
Priority to US07/468,008 priority patent/US5181971A/en
Publication of JPH0529122B2 publication Critical patent/JPH0529122B2/ja
Granted legal-status Critical Current

Links

Description

【発明の詳細な説明】[Detailed description of the invention]

〔産業上の利用分野〕 本発明は、複写機やプリンター等に用いられる
磁気ブラシ現像ローラに用いられる樹脂磁石であ
るマグネツトローラー及びその製造方法に関する
ものである。 〔従来の技術〕 従来より複写機やその他の機器に使用されるマ
グネツトローラとしては、等方性あるいは異方性
の焼結マグネツトや、樹脂マグネツトを芯金に貼
り付けたり圧入したものが一般的であつた。又、
近年に於いては、射出成形法による特公昭39−
28287や特公昭56−5045の応用により内部に極異
方性配向一体成形を行なつた特開昭56−108207な
ど多数の出願がなされている。 しかしながら、従来例に於ける焼結マグネツト
の貼り合せにあつては、欠けやすい、接着に手間
がかかるコストが高い等の問題があつた。さらに
焼結一体成形マグネツトに於いても焼き割れ、ソ
リ等により歩留まりが悪い、寸法精度が出ない等
の問題が有り、さらに重い、2次加工によりコス
トが高い等の問題はまぬがれなかつた。又、ゴ
ム、プラスチツクによる樹脂磁石の貼り合せにあ
つても、やはり接着、2次加工等によりコストが
高い等の問題があつた。その為近年に於ては、樹
脂磁石による一体成形のものも出現している。し
かし、等方性のものに於いては、磁力が不足して
いるのが現状である。そこでマグネツトローラー
の異方性化が多数試みられている。 〔発明が解決しようとする問題点〕 しかし、長尺で中実又は中空のマグネツトロー
ラーに於いては、ラジアル配向が不可能な為に、
モーター用ローラで試みられている極異方性配向
や2極配向の応用による一体化が一般的に行なわ
れている。 極異方性配向品の模式断面図を第11図に示し
てある。このように極異方性配向させるには多数
の磁極を成形品の周囲に配置した装置を用いるた
め装置が複雑なものになり製造費用が高くついて
いた。また11図に示すように表面近の磁性粉が
主に配向され中心部の磁性粉が配向されないため
表面磁束密度の分布がシヤープでなくその値も小
さいという問題点があつた。 また2極配向品の模式断面図を第10図に、そ
の製造過程を第9図に示した。上記のような極異
方性配向の場合は、マグネツトローラーのほとん
どの体積を有効に使用する為に特に多極にしない
限り金型に於いても、磁気効率が良く配向度を上
げることが可能である。しかし、2極配向多極着
磁の場合、第9図のような一様に平行な磁界を用
いて配向する為に第10図に示す様な成形品とな
つてしまう。その為に、マグネツトローラー内の
磁性粉個々のもつエネルギーが、表面磁束として
高い値を必要とする所に対しては、すべてが直線
上にあるわけではなくマグネツト上の磁極位置か
ら少し離れた位置に於いては、表面磁束密度が必
要な位置とは磁路として方向がずれてしまう為に
結果としては磁気効率はラジアル配向と同様の様
に配向度は高くても、ベクトルがずれている分布
低下してしまい、着磁の際もそのはずれた部分に
ついては磁路ではないのでベクトルがずれてしま
い各磁性粉が発揮できる磁力の最大値までフル着
磁されないために一見良さそうでも結果的には磁
力が極異方性配向よりもかなり劣つてしまう欠点
がある。 本発明は上記問題点に鑑み成されたものであり
その目的は、磁力が強く製造コストも低いマグネ
ツトローラー及びその製造方法を提供することに
ある。 〔問題点を解決する手段〕 本発明の上記目的は、磁性粉を含む樹脂材料か
ら成形配向された成形品からなるマグネツトロー
ラーであつて、 前記マグネツトローラーの軸に対して直角な断
面におけるローラー周辺部に、対向する一対の起
磁極と終磁極からなる磁極対の3つ以上を構成す
る複数の磁極を有し、 前記磁極は、それぞれの各磁極対における起磁
極と終磁極を結ぶ直線が前記断面上において互い
にほぼ平行となり、かつ隣り合う磁極は異なる磁
性を有するように配置されており、 しかも前記磁性粉が、前記マグネツトローラー
断面の周辺部において各磁極の磁気的ピークの中
心に向かつて収束する方向に配向されており、 前記ローラー断面の中心部分においては前記各
磁極対の起磁極と終磁極を結ぶ直線にほぼ平行に
成るように配向されている ことを特徴とするマグネツトローラー及びその製
造方法によつて達成される。 本発明のマグネツトローラーの1態様例の模式
断面図を第1図に示す。この態様においてはマグ
ネツトローラーは円筒形であり、その円周面上に
はN極(起磁極)の磁気ピークとS極(終磁極)
の磁気ピークとからなる磁性対が3つ設けられて
おり、N極とS極は円周面上で交互になるように
着磁されている。そして各々の磁性対のS極とN
極を結ぶ直線は第1図の平面上において平行とな
つている。しかしこの磁性対の位置関係は目的物
に合わせて平行でないように設けてもよい。また
その形状も円筒形に限らず任意の筒型をとりう
る。 この磁性対のN極とS極の間において強磁性体
粉末は第1図に示すように成形品中央部において
はN極とS極を結ぶ線に添つてほぼ平行に配向さ
れており、N極、S極近傍部すなわち円周面近く
にあつてはN極、S極の磁気的ピークの中心部に
向かつて収束するように配向されている。このよ
うな配向のため磁力はそれぞれの極の中心部に向
かつて強力に発生し第6図に示すようなシヤープ
な磁気ピークが得られる。この磁気ピークの大き
さも第6図のように全て同じである必要はなく、
所望に応じて異なる大きさにすればよい。 本発明のマグネツトローラーの材料としては従
来公知の材料が使用される。 以上の構成を有するマグネツトローラーの製造
に利用できる本発明のマグネツトローラーの製造
方法は、 a) 前記マグネツトローラー成形用のキヤビテ
イーを有し、該キヤビテイーの軸方向の断面の
外周部に前記キヤビテイーを挟んで、一方の外
周部に起磁極を配置し、他方の外周部に前記起
磁極と対を成す終磁極を配置し、前記各磁極対
の起、終磁極はキヤビテイーの中心部を通る磁
力線がほぼ平行になるように配置した成形用金
型を準備し、 b) 前記金型内にマグネツトローラー成形用の
磁性粉を含む樹脂材料を注入し、前記樹脂材料
内の磁性粉は、前記キヤビテイー外周部に配置
した前記磁極により磁気配向を受けて、キヤビ
テイー内の前記起、終磁極近傍の磁性粉は各磁
極の磁気的ピークの中心に向つて収束する方向
に配向され、前記キヤビテイー内の中心部の磁
性粉は前記各磁極対から発生されたほぼ平行な
磁束に対応してほぼ平行に配向されたローラー
状成形品を得る工程と、 c) 前記工程で得られたローラー状成形品の隣
り合う磁極が異なるように着磁する工程と を有することを特徴とする。 なお、着磁工程c)は、工程b)で得られたロ
ーラー状成形品をそのまま所望の磁極配置が得ら
れるように着磁することによつて、あるいは工程
b)で得られたローラー状成形品の磁性を一旦脱
磁した後、所望の磁極配置が得られるよう再着磁
することによつて行うことができる。 なお、着磁工程b)において脱磁を行わない場
合、脱磁工程を省略できるという利点がある。 また、工程a)で得られたローラー状成形品を
直接着磁する際に、大型でかつ高価な強力な着磁
装置が必要となる場合には、脱磁した後再着磁す
る方法を用いることは、強力な着磁装置を用いる
ことなく、良好な磁気特性を最終製品に得ること
ができるという点で有用である。 ローラー状成形品の着磁に際しては、磁性粉の
配向に沿つて着磁用の磁束がかかるように、例え
ば第6図に示すように、ローラー状成形品の成形
時における磁極と着磁用の磁極とを位置合せして
着磁が行われる。 以下、本発明のマグネツトローラについて、そ
の製造を挙げることにより更に詳細に説明する。 第2図〜第4図及び第6図は製造例の各工程
を、そして第8図は製造に用いた金型を模式的に
示すものである。また第9図及び第10図は従来
のマグネツトローラーを説明するものである。 第2図は製造例で用いた金型の金型内キヤビテ
イーまわりの図面であり、同図に於いて、1なら
びに4はキヤビテイーをはさんで対向した強磁性
材で構成した磁極であり、第8図において24な
らびに18で示す磁場発生用コイルからの磁束を
25,20で示す成形機プラテンを通して金型キ
ヤビテイーまで誘導するためのものである。さら
に7,8,9及び10,11,12は、上記1な
らびに4の磁極と一体に構成された磁極であり、
14で示す円筒形のキヤビテイー空間をはさんで
ほぼ対向させた状態に配置されている。すなわち
磁力線が流れ出す起磁極である7,8,9と磁力
線が流れ込む終磁極10,11,12とが向かい
合つて並んでおり、7と10、8と11,9と1
2がそれぞれ磁極対を形成しており7と10を結
ぶ線、8と11を結ぶ線、9と12を結ぶ線がほ
ぼ同一平面上にありほぼ平行となる様に各磁極が
配置されている。ここで各磁極は従来公知である
ような強磁性材で構成されている。また2,3,
5,6は非磁性材で構成されたスペーサーであ
る。 このような第8図の構成において18,24で
示す磁場発生用コイルに電流を流すと、そこで発
生した磁束(磁力線)は、20の可動側成形機プ
ラテンを通つて金型内の強磁性材料で構成された
1の磁極から、7,8,9の磁極(起磁極)に分
かれ、14のキヤビテイー内に流れ込み第2図に
13で示す様にギヤツプ間のパーミアンスの分布
に従つて流れ、対向する10,11,12の磁極
(終磁極)に集まるように流れる。すなわち、各
磁極近傍以外では同一方向の互いにほぼ平行な磁
束がキヤビテイー内に発生する。その磁束は4の
磁極を通して第8図の25で示す固定側プラテン
を通つて、19で示すタイバーを通り、閉ループ
となるように構成されている。 以上のように磁束が閉ループを形成している状
態に於いて、溶融させた樹脂磁石材料(強磁性体
粉末とバインダー)を14のキヤビテイーに射出
注入を行なうと、第3図に示すように磁性粉15
の配向が第2図で示した磁力線の流れに従つて起
こる。磁力線は第2図に示すようキヤビテイー内
においては広がり磁極部分においては収束するた
め、磁性粉も第3図で示すように磁極部分におい
て収束した状態に配向される。このような配向の
ため成形品内部の磁性粉が有効に用いられ、成形
品の所望の位置に磁力線が集中されるため、表面
磁束密度の高い、磁力の強いマグネツトローラー
を得ることができる。第3図に示すような磁性粉
の配向状態を保持しつつ冷却固化させて、取り出
すと第4図に示す成形品が得られる。その際の第
4図に示す成形品の表面磁束密度の分布は第5図
上段に示す様になる。 次に第4図で示した成形品を従来公知の方法に
より一旦脱磁し、配向はそのまま固定したまま、
磁気だけを取り去る。次に第6図に示す様にヨー
ク16と着磁コイル17を主体とする着磁器にて
順次着磁し直すことにより第1図に着磁状態を示
すような成形品が得られる。このときの表面磁束
密度の分布を第5図下段に示す。成形品の各磁性
対のN極とS極間の距離は異なるため、円周面上
の全ての極の磁気ピークの大きさを同じにするた
めには、着磁器のヨークの材質又は断面積(ある
いは用いる電流の大きさ)を変えることにより、
N極S極間において強磁性体粉末が配向している
部分の巾を変化させて配向している強磁性体粉末
の数を調整すればよい。また配向している強磁性
体粉末の数を調整して磁気ピークの大きさを故意
に異ならさせてもよい。第6図に示すような着磁
器で容易に確実に着磁が行なわれるのは、第1図
のように成形品中での配向がN極S極間の磁力線
の流れに添うようにそれぞれの磁性対について独
立明確になされているためであり、第9図で示す
ような従来の2極配向品では明確な磁気ピークが
得られるとは考えられない。 前記と同様の方法で4極と6極のプラスチツク
マグネツトローラーを作成し、その評価を行つ
た。なお4極の配向については第7図に示してあ
るように行つた。評価は最大表面磁束密度900
〔G〕以上、半減時幅60%以下という複写機用現
像ローラーとして一般的に必要な代表スペツクと
比較する。なお半減時幅は第12図に示すA,B
を用いて下記式で表される。 半減時幅=(A/B)×100〔%〕 (この値が大きいほど波形が広がつている) テスト1として本発明の4極マグネツトローラ
ー及び従来の極異方性配向品及び2極配向品を試
験し、テスト2として本発明の6極マグネツトロ
ーラー及び従来の極異方性配向品及び2極配向品
を試験し、その結果を第1表、第2表に示した。
なおいずれの試料も、材料としては公知のプラス
チツクマグネツト材料にストロンチウムフエライ
トを90wt%混合させたものを用い、金型温度110
℃、成形温度280℃で射出成形を行なうことによ
りφ=20mmと14mmの2種類のマグネツトローラー
を製造した。
[Industrial Application Field] The present invention relates to a magnet roller, which is a resin magnet used in a magnetic brush developing roller used in copying machines, printers, etc., and a method for manufacturing the same. [Prior art] Magnet rollers conventionally used in copying machines and other equipment have generally been made of isotropic or anisotropic sintered magnets or resin magnets pasted or press-fitted onto a core metal. It was spot on. or,
In recent years, the injection molding method has been used to produce
A large number of applications have been filed, including JP-A No. 56-108207, in which polar anisotropic orientation integral molding is performed internally by applying Patent Publication No. 28287 and JP-B No. 56-5045. However, in bonding sintered magnets in the conventional example, there were problems such as easy chipping, troublesome bonding, and high cost. Furthermore, sintered integrally molded magnets also have problems such as poor yields and poor dimensional accuracy due to quenching cracks and warping, as well as problems such as being heavy and requiring high costs due to secondary processing. Further, even when bonding resin magnets with rubber or plastic, there are still problems such as high cost due to adhesion, secondary processing, etc. For this reason, in recent years, one-piece molded magnets made of resin magnets have also appeared. However, isotropic materials currently lack magnetic force. Therefore, many attempts have been made to make magnetic rollers anisotropic. [Problems to be solved by the invention] However, since radial orientation is impossible with long, solid or hollow magnetic rollers,
Integration by applying polar anisotropic orientation or bipolar orientation, which has been attempted in motor rollers, is generally performed. A schematic cross-sectional view of the polar anisotropically oriented product is shown in FIG. In order to achieve polar anisotropic orientation in this manner, a device in which a large number of magnetic poles are arranged around the molded product is used, which makes the device complicated and increases manufacturing costs. Furthermore, as shown in FIG. 11, the magnetic powder near the surface is mainly oriented and the magnetic powder in the center is not oriented, so there is a problem that the surface magnetic flux density distribution is not sharp and its value is small. Further, a schematic cross-sectional view of the bipolar oriented product is shown in FIG. 10, and the manufacturing process thereof is shown in FIG. In the case of polar anisotropic orientation as described above, in order to effectively use most of the volume of the magnetic roller, it is possible to improve the magnetic efficiency and increase the degree of orientation even in the mold unless the magnetic roller is multipole. It is possible. However, in the case of bipolar orientation multipolar magnetization, since orientation is performed using a uniformly parallel magnetic field as shown in FIG. 9, a molded product as shown in FIG. 10 is obtained. For this reason, in areas where the energy of each magnetic powder in the magnet roller requires a high value as surface magnetic flux, the energy of each magnetic powder in the magnet roller is not all in a straight line, but is located a little far from the magnetic pole position on the magnet. In terms of position, the direction of the magnetic path differs from the position where the surface magnetic flux density is required, so as a result, although the magnetic efficiency is similar to radial orientation and the degree of orientation is high, the vector is shifted. The distribution decreases, and when magnetizing, the deviated part is not a magnetic path, so the vector is shifted, and each magnetic powder is not fully magnetized to the maximum value of magnetic force that it can exert, so even if it looks good at first glance, the result is has the disadvantage that the magnetic force is considerably inferior to that of polar anisotropic orientation. The present invention has been made in view of the above-mentioned problems, and its object is to provide a magnet roller with strong magnetic force and low manufacturing cost, and a method for manufacturing the same. [Means for Solving the Problems] The above-mentioned object of the present invention is to provide a magnet roller comprising a molded article molded and oriented from a resin material containing magnetic powder. The peripheral portion of the roller has a plurality of magnetic poles constituting three or more magnetic pole pairs consisting of a pair of opposing magnetomotive poles and a final magnetization pole, and the magnetic poles are formed by a straight line connecting the magnetomotive pole and the final magnetization pole of each magnetic pole pair. are arranged so that they are substantially parallel to each other on the cross section, and adjacent magnetic poles have different magnetic properties, and the magnetic powder is located at the center of the magnetic peak of each magnetic pole in the periphery of the cross section of the magnet roller. The magnet is oriented in a direction in which the magnets and magnets converge, and the magnet is oriented in a central portion of the cross section of the roller so as to be substantially parallel to a straight line connecting the magnetizing pole and the final magnetizing pole of each pair of magnetic poles. This is achieved by a roller and its manufacturing method. A schematic sectional view of one embodiment of the magnetic roller of the present invention is shown in FIG. In this embodiment, the magnet roller has a cylindrical shape, and on its circumferential surface there is a magnetic peak of an N pole (magnetizing pole) and an S pole (final magnetizing pole).
Three magnetic pairs consisting of magnetic peaks are provided, and the north and south poles are magnetized alternately on the circumferential surface. And the S pole and N pole of each magnetic pair
The straight lines connecting the poles are parallel on the plane of FIG. However, the positional relationship of this magnetic pair may be arranged so as not to be parallel depending on the object. Further, its shape is not limited to a cylindrical shape, but can be any cylindrical shape. As shown in Figure 1, the ferromagnetic powder between the north and south poles of this magnetic pair is oriented almost parallel to the line connecting the north and south poles in the center of the molded product, and the Near the poles and south poles, that is, near the circumferential surface, they are oriented so as to converge toward the center of the magnetic peaks of the north and south poles. Because of this orientation, a strong magnetic force is generated toward the center of each pole, resulting in a sharp magnetic peak as shown in FIG. The size of these magnetic peaks does not have to be the same as shown in Figure 6.
It may be made to have a different size as desired. Conventionally known materials can be used for the magnetic roller of the present invention. The method for manufacturing a magnetic roller of the present invention, which can be used to manufacture a magnetic roller having the above configuration, includes a) a cavity for molding the magnetic roller, and the outer circumference of the axial cross section of the cavity has the A magnetizing pole is arranged on one outer periphery of the cavity, and a final magnetizing pole that pairs with the magnetizing pole is arranged on the other outer periphery, and the starting and final magnetizing poles of each pair of magnetic poles pass through the center of the cavity. Prepare a molding mold arranged so that the lines of magnetic force are almost parallel, b) Inject a resin material containing magnetic powder for molding a magnet roller into the mold, and the magnetic powder in the resin material: Being magnetically oriented by the magnetic poles arranged on the outer periphery of the cavity, the magnetic powder in the vicinity of the starting and ending poles in the cavity is oriented in a direction converging toward the center of the magnetic peak of each magnetic pole. c) obtaining a roller-shaped molded product in which the magnetic powder at the center of the magnetic powder is oriented substantially parallel in response to the substantially parallel magnetic flux generated from each of the magnetic pole pairs; c) the roller-shaped molded product obtained in the step; The method is characterized by comprising a step of magnetizing so that adjacent magnetic poles are different from each other. Note that the magnetization step c) is performed by directly magnetizing the roller-shaped molded product obtained in step b) so as to obtain the desired magnetic pole arrangement, or by magnetizing the roller-shaped molded product obtained in step b). This can be done by once demagnetizing the item and then re-magnetizing it to obtain the desired magnetic pole arrangement. Note that when demagnetization is not performed in the magnetization step b), there is an advantage that the demagnetization step can be omitted. In addition, if a large, expensive, and powerful magnetizing device is required to directly magnetize the roller-shaped molded product obtained in step a), a method of demagnetizing and then re-magnetizing is used. This is useful in that good magnetic properties can be obtained in the final product without using a powerful magnetization device. When magnetizing a roller-shaped molded product, for example, as shown in Figure 6, the magnetic pole and the magnetization flux are aligned so that the magnetic flux for magnetization is applied along the orientation of the magnetic powder. Magnetization is performed by aligning the magnetic poles. Hereinafter, the magnet roller of the present invention will be explained in more detail by mentioning its manufacture. 2 to 4 and 6 schematically show each step of the manufacturing example, and FIG. 8 schematically shows the mold used in the manufacturing. Further, FIGS. 9 and 10 illustrate a conventional magnetic roller. Figure 2 is a drawing of the cavity in the mold used in the manufacturing example. In the figure, 1 and 4 are magnetic poles made of ferromagnetic material facing each other with the cavity in between. This is for guiding the magnetic flux from the magnetic field generating coils shown at 24 and 18 in FIG. 8 through the molding machine platens shown at 25 and 20 to the mold cavity. Further, 7, 8, 9 and 10, 11, 12 are magnetic poles that are integrated with the magnetic poles 1 and 4 above,
They are arranged substantially facing each other across a cylindrical cavity space indicated by 14. That is, magnetomotive poles 7, 8, and 9 from which lines of magnetic force flow and final poles 10, 11, and 12, into which lines of magnetic force flow, are lined up facing each other.
2 form a magnetic pole pair, and each magnetic pole is arranged so that the line connecting 7 and 10, the line connecting 8 and 11, and the line connecting 9 and 12 are almost on the same plane and are almost parallel. . Here, each magnetic pole is constructed of a ferromagnetic material as is conventionally known. Also 2, 3,
5 and 6 are spacers made of non-magnetic material. When current is applied to the magnetic field generating coils 18 and 24 in the configuration shown in FIG. The magnetic pole 1 is divided into 7, 8, and 9 magnetic poles (magnetomotive poles), and the flow flows into the 14 cavities according to the permeance distribution between the gaps, as shown at 13 in Figure 2. The flow converges at magnetic poles 10, 11, and 12 (final magnetic poles). That is, magnetic fluxes that are substantially parallel to each other in the same direction are generated within the cavity except in the vicinity of each magnetic pole. The magnetic flux passes through the magnetic pole 4, passes through the stationary platen shown at 25 in FIG. 8, and passes through the tie bar shown at 19, forming a closed loop. With the magnetic flux forming a closed loop as described above, when molten resin magnet material (ferromagnetic powder and binder) is injected into the 14 cavities, magnetic powder 15
The orientation of the magnetic field occurs according to the flow of the magnetic field lines shown in FIG. Since the lines of magnetic force spread within the cavity as shown in FIG. 2 and converge at the magnetic pole portion, the magnetic powder is also oriented in a converged state at the magnetic pole portion as shown in FIG. 3. Because of this orientation, the magnetic powder inside the molded product is effectively used and the lines of magnetic force are concentrated at desired positions of the molded product, so that a magnetic roller with a high surface magnetic flux density and strong magnetic force can be obtained. When the magnetic powder is cooled and solidified while maintaining its orientation as shown in FIG. 3, and taken out, a molded article shown in FIG. 4 is obtained. At this time, the distribution of surface magnetic flux density of the molded product shown in FIG. 4 becomes as shown in the upper part of FIG. 5. Next, the molded product shown in Fig. 4 was demagnetized by a conventionally known method, and the orientation was fixed as it was.
Only the magnetism is removed. Next, as shown in FIG. 6, the molded product as shown in the magnetized state shown in FIG. 1 is obtained by sequentially re-magnetizing it using a magnetizer mainly consisting of a yoke 16 and a magnetizing coil 17. The distribution of surface magnetic flux density at this time is shown in the lower part of FIG. Since the distance between the N and S poles of each magnetic pair of the molded product is different, in order to make the magnetic peaks of all the poles on the circumferential surface the same, it is necessary to change the material or cross-sectional area of the yoke of the magnetizer. (or by changing the magnitude of the current used)
The number of oriented ferromagnetic powders may be adjusted by changing the width of the portion where ferromagnetic powders are oriented between the north and south poles. Alternatively, the magnitude of the magnetic peak may be intentionally varied by adjusting the number of oriented ferromagnetic powders. The reason why magnetization is easily and reliably carried out using the magnetizer shown in Figure 6 is that the orientation in the molded product follows the flow of the magnetic field lines between the north and south poles, as shown in Figure 1. This is because the magnetic pairs are independent and clearly defined, and it is unlikely that a clear magnetic peak can be obtained with a conventional bipolar alignment product as shown in FIG. Four-pole and six-pole plastic magnetic rollers were prepared in the same manner as described above, and evaluated. Note that the orientation of the four poles was performed as shown in FIG. Rating is maximum surface magnetic flux density 900
[G] Compare the above with the typical specifications generally required for a developing roller for a copying machine, which is 60% or less width at half-life. The half-life time widths are A and B shown in Figure 12.
It is expressed by the following formula using . Width at half-life = (A/B) x 100 [%] (The larger this value is, the wider the waveform is.) As test 1, the 4-pole magnetic roller of the present invention, the conventional polar anisotropically oriented product, and the 2-pole The oriented products were tested, and as Test 2, the 6-pole magnetic roller of the present invention, the conventional polar anisotropically oriented product, and the bipolar oriented product were tested, and the results are shown in Tables 1 and 2.
All samples were made using a well-known plastic magnet material mixed with 90wt% strontium ferrite, and the mold temperature was 110%.
Two types of magnetic rollers with a diameter of 20 mm and 14 mm were manufactured by injection molding at a molding temperature of 280 °C.

【表】【table】

〔発明の効果〕〔Effect of the invention〕

以上説明したように、本発明のマグネツトロー
ラーは表面磁束密度の磁気ピークがシヤープ、す
なわち半減時幅が小さく、表面磁束密度の値も大
きいため優れた性能を有する。また中心部分の磁
性粉も磁力発生に寄与しており磁力に余裕のある
だけ小径化することができる。また製造に使用す
る装置も小型簡単なものでよい。
As explained above, the magnetic roller of the present invention has excellent performance because the magnetic peak of the surface magnetic flux density is sharp, that is, the width at half-life is small, and the value of the surface magnetic flux density is large. In addition, the magnetic powder in the center part also contributes to the generation of magnetic force, and the diameter can be made as small as there is enough magnetic force. Furthermore, the equipment used for manufacturing may be small and simple.

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

第1図は着磁後のマグネツトローラーの断面
図、第2図は本発明のマグネツトローラーの製造
に用いられる金型のキヤビテイー近傍の断面図、
第3図はキヤビテイーに樹脂磁石材料を射出注入
配向した状態の断面図、第4図は、成形取り出し
後のマグネツトローラーの断面図、第5図はマグ
ネツトローラーの周面の磁束分布グラフ(第5図
の上段は成形取り出し後における磁束分布を、下
段は着磁後の磁束分布をそれぞれ示す)、第6図
は着磁器を用いて再着磁している様子を表す模式
図、第7図は第3図において磁極を4極としたも
のの断面図、第8図は製造例に用いた磁場射出成
形装置と金型部を示す模式図、第9図は従来の2
極配向を説明する模式図、第10図は2極配向品
を脱磁後再着磁したマグネツトローラーの断面
図、第11図は極異方性配向品の断面図、第12
図は半減時幅を説明する図、第13図は本発明の
マグネツトローラーを現像機に装着している部分
図である。 1,4……磁極、2,3,5,6……磁極(非
磁性材)、7,8,9……磁極(起磁極)、10,
11,12……磁極(終磁極)、13……磁束
(磁力線)の流れ、14……金型内のキヤビテイ
ー、15……磁性粉、16……ヨーク、17……
着磁コイル、18,24……磁場発生用コイル、
20……可動側成形機プラテン、21……固定側
金型、23……可動側金型、25……固定側成形
機プラテン、26,27,28……磁極。
FIG. 1 is a sectional view of the magnetic roller after magnetization, FIG. 2 is a sectional view of the vicinity of the cavity of the mold used for manufacturing the magnetic roller of the present invention,
Fig. 3 is a cross-sectional view of the resin magnet material injected and oriented into the cavity, Fig. 4 is a cross-sectional view of the magnet roller after being removed from the mold, and Fig. 5 is a graph of the magnetic flux distribution on the circumferential surface of the magnet roller ( (The upper part of Figure 5 shows the magnetic flux distribution after demolding, and the lower part shows the magnetic flux distribution after magnetization.) Figure 6 is a schematic diagram showing re-magnetization using a magnetizer, and Figure 7 The figure is a cross-sectional view of the magnetic field injection molding device with four magnetic poles in Figure 3, Figure 8 is a schematic diagram showing the magnetic field injection molding device and mold part used in the manufacturing example, and Figure 9 is a conventional 2-pole model.
A schematic diagram for explaining polar orientation, FIG. 10 is a sectional view of a magnet roller obtained by demagnetizing and remagnetizing a bipolar oriented product, FIG. 11 is a sectional view of a polar anisotropically oriented product, and FIG.
The figure is a diagram for explaining the width at half-life, and FIG. 13 is a partial view of the magnetic roller of the present invention installed in a developing machine. 1, 4... Magnetic pole, 2, 3, 5, 6... Magnetic pole (non-magnetic material), 7, 8, 9... Magnetic pole (magnetic pole), 10,
11, 12... Magnetic pole (final magnetic pole), 13... Flow of magnetic flux (magnetic field lines), 14... Cavity in the mold, 15... Magnetic powder, 16... Yoke, 17...
Magnetizing coil, 18, 24...magnetic field generation coil,
20...Movable side molding machine platen, 21...Fixed side mold, 23...Movable side mold, 25...Fixed side molding machine platen, 26, 27, 28...Magnetic pole.

【特許請求の範囲】[Claims]

1 内胴の両端部にフランジを有する巻枠に超電
導巻線とクエンチ促進用ヒータが設けられたもの
において、両フランジの内側面にスペーサを介し
て少なくとも円周方向に2個以上に分割された円
環板状のクエンチ促進用ヒータを配設し、さらに
このクエンチ促進用ヒータの内側面に絶縁部材を
介して内胴の外周に超電導巻線を巻回したことを
特徴とする超電導マグネツト。
1 In a case where a superconducting winding and a quench promotion heater are installed on a winding frame having flanges at both ends of the inner shell, the coil frame is divided into two or more pieces at least in the circumferential direction with a spacer on the inner surface of both flanges. A superconducting magnet characterized in that a circular plate-shaped quench promoting heater is disposed, and a superconducting winding is further wound around the outer periphery of an inner shell on the inner surface of the quench promoting heater with an insulating member interposed therebetween.

Claims (1)

前記磁極は、それぞれの各磁極対における起磁
極と終磁極を結ぶ直線が前記断面上において互い
にほぼ平行となり、かつ隣り合う磁極は異なる磁
性を有するように配置されており、 しかも、磁性粉が、前記断面の周辺部において
各磁極の磁気的ピークの中心に向つて収束する方
向に配向されており、 前記断面の中心部分においては前記各磁極対の
起磁極と終磁極を結ぶ直線にほぼ平行に成るよう
に配向されているマグネツトローラーの製造方法
であつて、 a) 前記マグネツトローラー成形用のキヤビテ
イーを有し、該キヤビテイーの軸方向の断面の
外周部に前記キヤビテイーを挟んで、一方の外
周部に起磁極を配置し、他方の外周部に前記起
磁極と対を成す終磁極を配置し、前記各磁極対
の起、終磁極はキヤビテイーの中心部を通る磁
力線がほぼ平行になるように配置した成形用金
型を準備し、 b) 前記金型内にマグネツトローラー成形用の
磁性粉を含む樹脂材料を注入し、前記樹脂材料
内の磁性粉は、前記キヤビテイー外周部に配置
した前記磁極により磁気配向を受けて、キヤビ
テイー内の前記起、終磁極近傍の磁性粉は各磁
極の磁気的ピークの中心に向つて収束する方向
に配向され、前記キヤビテイー内の中心部の磁
性粉は前記各磁極対から発生されたほぼ平行な
磁束に対応してほぼ平行に配向されたローラー
状成形品を得る工程と、 c) 前記工程で得られたローラー状成形品の隣
り合う磁極が異なるように着磁する工程と を有することを特徴とするマグネツトローラーの
製造方法。
The magnetic poles are arranged such that straight lines connecting the magnetizing pole and the final magnetizing pole in each pair of magnetic poles are substantially parallel to each other on the cross section, and adjacent magnetic poles have different magnetisms, and the magnetic powder is It is oriented in a direction that converges toward the center of the magnetic peak of each magnetic pole in the peripheral part of the cross section, and is oriented almost parallel to a straight line connecting the magnetizing pole and the final magnetizing pole of each magnetic pole pair in the central part of the cross section. A method for manufacturing a magnetic roller oriented so that the magnet roller is formed, the method comprising: a) having a cavity for molding the magnetic roller, sandwiching the cavity at the outer circumference of the axial cross section of the cavity, and forming one of the magnetic rollers; A magnetizing pole is arranged on the outer periphery, and a final magnetizing pole that pairs with the magnetizing pole is arranged on the other outer periphery, and the starting and final magnetizing poles of each pair of magnetic poles are arranged so that lines of magnetic force passing through the center of the cavity are almost parallel. a) a resin material containing magnetic powder for magnetic roller molding is injected into the mold, and the magnetic powder in the resin material is arranged on the outer periphery of the cavity; Under magnetic orientation by the magnetic poles, the magnetic powder near the starting and ending poles in the cavity are oriented in a direction converging toward the center of the magnetic peak of each magnetic pole, and the magnetic powder in the center of the cavity is c) obtaining a roller-shaped molded product oriented substantially parallel in response to the substantially parallel magnetic fluxes generated from each pair of magnetic poles; c) so that adjacent magnetic poles of the roller-shaped molded product obtained in the step are different; 1. A method for manufacturing a magnetic roller, comprising the step of magnetizing the roller.
JP2558587A 1986-05-20 1987-02-07 Magnet roller Granted JPS6464204A (en)

Priority Applications (3)

Application Number Priority Date Filing Date Title
JP2558587A JPS6464204A (en) 1987-02-07 1987-02-07 Magnet roller
US07/049,966 US4954800A (en) 1986-05-20 1987-05-15 Magnet and method of manufacturing the same
US07/468,008 US5181971A (en) 1986-05-20 1990-01-22 Magnet and method of manufacturing the same

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2558587A JPS6464204A (en) 1987-02-07 1987-02-07 Magnet roller

Publications (2)

Publication Number Publication Date
JPS6464204A JPS6464204A (en) 1989-03-10
JPH0529122B2 true JPH0529122B2 (en) 1993-04-28

Family

ID=12169992

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2558587A Granted JPS6464204A (en) 1986-05-20 1987-02-07 Magnet roller

Country Status (1)

Country Link
JP (1) JPS6464204A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109419391A (en) * 2017-08-31 2019-03-05 佛山市顺德区美的电热电器制造有限公司 Disk mounting assembly and food processor

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CS213709B1 (en) * 1979-03-13 1982-04-09 Vaclav Landa Anizotropous permanent magnets
JPS61112310A (en) * 1984-11-07 1986-05-30 Sumitomo Bakelite Co Ltd Manufacture of permanent magnet

Also Published As

Publication number Publication date
JPS6464204A (en) 1989-03-10

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