JPH0533802B2 - - Google Patents
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- JPH0533802B2 JPH0533802B2 JP62025584A JP2558487A JPH0533802B2 JP H0533802 B2 JPH0533802 B2 JP H0533802B2 JP 62025584 A JP62025584 A JP 62025584A JP 2558487 A JP2558487 A JP 2558487A JP H0533802 B2 JPH0533802 B2 JP H0533802B2
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Description
〔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の製造方法及びそれに用い
得る金型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
グネツトローラーとしては、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。極異方性配向に於いては、金型内や金
型外にコイルを配置したり、又、永久磁石を配置
したりする方法が提案されているが実用上、下記
の問題がある。
パルス磁界を発生するコイルを金型に内蔵し
た方式については、装置的には小型で済み理想
的であるが、パルス幅が短い為に、配向度が向
上せず高性能のものが得られない。特に静電現
象用マグネツトローラーに於いては高い表面磁
束密度が要求される為に磁性粉の含有量の高い
ものを使用する為に成形材料のみかけ粘度が非
常に高くパルス磁界で配向することは現実的に
は、ほとんど不可能であつた。
永久磁石を金型内に内蔵した方式について
は、装置的には割り合い小型で済み有効である
が、やはりマグネツトローラーに於いては、成
形材料の粘度が高い為に磁性粉を完全に配向さ
せることができなかつた。又、量産上に於いて
成形品が金型に強く吸い付けられる為に、金型
から離型させる際完全に冷却するまでサイクル
を長くしないとソリ等の変形を起こし、歩留ま
りが非常に悪くなり量産上は、効率が悪く問題
があつた。
静磁界を発生するコイルを金型に内蔵する方
式については、2極より多極にして極異方性配
向させた場合、金型内の磁極の配置が第9図に
示す様に様々な方向に向いて並べられる為にパ
ーテイングライン上にキヤビテイーを並べられ
ず、キヤビテイーまわりの必要スペースが大き
くなり、さらにコイルを内蔵する大きなスペー
スが必要となる。又、その為に取個数が限定さ
れてしまい、やはり量産上、生産性が非常に悪
かつた。
静磁界を発生するコイルを金型の外に設置す
る場合についてもやはり、2極マグネツトより
多極にして極異方性配向させた場合にキヤビテ
イー近傍の磁極配置が上記と同様になり同様
の問題点があると共に、さらに金型外のコイル
へつなげる為の磁路が金型内外で広がる為に内
造タイプよりも1つのキヤビテイーを形成する
に必要なスペースが、いつそう広がつてしまう
問題があつた。その為やはり多数個取りが非常
に困難な為に生産性が非常に悪いという欠点を
有していた。
さらにマグネツトローラーの性能面において
極数が4極よりも多くなつた場合、極異方性配
向の欠点である配向度の低下が起こり、配向し
ている部分が表面層に近いところのみとなり、
中心に近い部分の磁性粉が有効利用されない為
に磁気効率が低下してしまう欠点がある。これ
は下記の2つの大きな原理的な欠点があるため
である。
a○ 第12図に示すように、極数が増加するに
従い極異方性配向の原理である磁気回路とな
る隣接する磁極対間において、それを最短距
離で結ぶ弦となる磁極ギヤツプ間のいちばん
磁場の強くかかる部分がキヤビテイーの中心
部に対して極数が増えるほど外側の表面方向
へ移動してしまうことである。この為に中心
部においては磁極のギヤツプ間のパーミアン
スによつて定義される非常に弱い漏で磁束に
よつてしか配向ができずマグネツトローラー
の様に磁性粉含有量の多いものにおいては材
料のみかけの粘土が非常に高いためにん完全
には磁性粉を配向できず特性が低下してしま
う欠点があつた。
b○ さらに磁極が増加するに従つて磁極対が対
向して配置されていないために、磁力線が隣
接する磁気回路となる磁極間のキヤビテイー
のギヤツプを通らずに第13図中に矢印で示
すように直接キヤビテイーのまわりの磁極間
でリークしてしまう欠点がある。このため金
型内の磁気回路としての効率が大きく低下し
てしまつていた。その結果やはり配向度が低
下してしまい特性が低下してしまう欠点があ
つた。
さらに静電現象用ではなくモーター用ロータ
ーの製造方法として2極で一方向に成形配向を
行ない多極に着磁に使用する方法が実公昭53−
38159や特開昭61−112310に開示されている。
これらによれば上記の金型内で磁極が多方向に
広がる問題点を一応解決することができると考
えることは記載されていないが容易に類推する
ことができる。しかし、これらの従来の方法に
於いては、静電現象用マグネツトローラーを製
造した場合には、以下のようないくつかの問題
点を有していた。
(A) 磁力が弱い。
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10図の要な一様に平行な磁
界を用いて配向する為に第11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
ル着磁されない為に一見良さそうでも結果的には
極異方性配向よりもかなり劣つてしまう欠点があ
る。
(B) 分布特性がコントロールできない。
又、静電現象用マグネツトローラーの必要特性
としては、上述の表面磁束密度の高さのほかに、
画像特性に特に影響を与えるものとして、そのマ
グネツトローラーから空間に放出している磁束の
分布特性の良悪がある。極異方性配向はこの点に
ついては問題がないが2極配向、多極着磁マグネ
ツトローラーに於いては、種々の欠点があること
がわかつた。つまり、マグネツトローラーとして
は、現象部分等に於いては、均一な真すぐに立つ
たトナーの穂立ちが必要であり、また急激に表面
磁束密度を円周方向分布に於いて部分的に高くし
たり低くしたりすることが設計的に必要である。
しかし、2極配向多極着磁を行なう方法に於いて
は、上述の様にそのマグネツトローラー上の必要
な磁極位置に於いて磁性粉の異方化方向が単一の
方向を向いているのみで必要な波形になる様に集
束していない為に表面磁束密度波形も単一の方向
を向いている磁性粉により一義的に決定されてし
まつた分布を持つてしまい、波形をうまく着磁ヨ
ークの形状と着磁の強弱だけでコントロールする
ことは非常に困難であつた。まして、表面磁束密
度の絶対値を上げる為にフルパワーで着磁を行な
い同時に分布波形をコントロールすることはまつ
たく不可能であつた。つまり、極異方性配向を応
用したマグネツトローラーに於いては、表面磁束
密度分布、高さを極数が少ない場合は同時に満た
すことはできても工業的には非常に生産性が低い
という欠点があり、2極配向多極着磁を応用した
マグネツトローラーに於いては、生産性は高くて
も表面磁束密度の高さ、分布特性をクリアーする
ものができないという欠点があつた。
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、磁性粉の含有量の多いものでも強力
かつ配向度よく配向し強い磁力を得ることが可能
であり、また表面磁束密度の高さ及び分布を制御
することができ、さらに歩留りが良く多数個取り
も可能で生産性が良い、マグネツトローラーの製
造方法及びそれに用い得る金型を提供することに
ある。
〔問題点を解決する手段〕
本発明の上記目的は、軸に対して直角な断面に
おける周辺部に、対向する一対の起磁極と終磁極
とからなる磁極対の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、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 起磁極と終磁極からなる配向用磁極対の複数
を、ローラー成形用キヤビテイーを挟んで一方
の側に起磁極が、他方の側に終磁極が並び、か
つ前記マグネツトローラーの磁極対の配置に対
応するように配置し、これら配向用磁極対から
同一方向の互いにほぼ平行な磁束をかけつつ該
キヤビテイーに注入された磁性粉を含む樹脂材
料を成形し、各配向用磁極に対応する位置に磁
極を有し、かつ前記磁性粉が各配向用磁極近傍
において各配向用磁極の磁気的ピークの中心に
向つて収束する方向で、それ以外の部分では各
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、
b 該工程aで得られたローラー状成形品の磁極
の一部の磁性を反転させ、隣りあう磁極が異な
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
の製造方法によつて達成される。
また、上記工程aに用い得る本発明の金型は、
磁性粉を含む樹脂材料を成形配向したマグネツト
ローラーを成形するために磁性材で作つたキヤビ
テイーの断面中心を通る線上の左右にそれぞれ配
向用起磁極部材と配向用終磁極部材を設け、
前記各磁極部材を少なくとも3分割するため
に、前記中心線に平行な長手形状の非磁極材で作
つたスペーサーを前記キヤビテイー断面中心線と
各スペーサーの長手方向が平行であつて、かつ、
前記各スペーサーの先端部がキヤビテイーの一部
を構成するように配置し、
前記起磁極部材からの磁力線は前記スペーサー
によつて分割されてキヤビテイー内の前記磁性粉
を、前記起磁極と前記終磁極を結ぶ直線上に沿つ
て前記断面において互いにほぼ平行となり、か
つ、各磁極の磁気的ピークの中心に向つて収束す
るように構成した
ことを特徴とする。
本発明の方法において、樹脂磁石材料(強磁性
体粉末とバインダー)としては従来公知のものが
使用されるが、成形配向の際に磁力線を成形品に
対し一方方向に流すことにより配向させる力が大
きいため、またマグネツトローラーの中心部の磁
性粉まで全て配向されるため、強磁性体粉末の含
有量の多い材料も難無く用いることができる。
本発明において、配向用磁力線をかけるための
磁極をなす強磁性材料の材質を変化させることに
より、また磁極の断面積を変化させることによ
り、あるいはその両方を変化させることにより成
形品の表面磁束密度を簡単に制御することができ
る。すなわち上述の方法により、各磁極間を通過
する磁束量を変化させて、成形品内部に於いて各
極に起こる磁気連鎖による配向された磁性粉の体
積比率そのものを変化させることにより、表面磁
束密度の分布コントロールが、着磁の強弱をつけ
ることなく、各極ともフル着磁の状態で行なわれ
マグネツトローラーの内部のすべての磁性粉の最
大エネルギーを取り出しながら行なえるわけであ
る。
以下、図面を参照にしつつ本発明を具体的に説
明する。
〔実施例〕
第1図〜第6図は本発明の実施例の各工程を模
式的に示すものである。また第9図〜第11図は
従来の実施例を示したものである。
第1図は本発明の特徴を最もよく表わす金型内
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性粉の配向用の磁極
(磁極部材)であり、第8図に示す成形機におい
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
部であり、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となる磁極
部である7,8,9と磁力線が流れ込む終磁極と
なる磁極部10,11,12とが向かい合つて並
んでおり、7と10,8と11,9と12がそれ
ぞれ磁極部対を形成しており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部が配置
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。
すなわち、第8図の成形機が有する金型は、キ
ヤビテイーを挟んで対向する一対の磁極1,4の
キヤビテイー側端部に非磁性材からなるスペーサ
ーで分割された磁極部を有することを特徴として
いる。
このような構成を金型が有することで、成形機
内におけるパーテイング部を挟んた両側に磁極部
を振り分けて配置できるようになり、成形機内に
パーテイング面に沿つて空間の余裕ができ、その
空間を利用して多数個取りを可能とする多数のキ
ヤビテイーの並列化を行なうことができる。
このような構成において第8図において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、2,8,9の磁極部(起磁
極)に分かれ、14のキヤビテイー内に流れ込み
第1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10,11,1
2の磁極(終磁極)に集まる用に流れる。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、
閉ループとなる用に構成されている。
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2図に示す用に磁性粉15の
配向が第1図で示した磁力線の流れに従つて起こ
る。磁力線は第1図で示すようキヤビテイー内に
おいては広がり磁極部においては収束するため、
磁性粉も第2図で示すように磁極部において収束
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2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
3図に示す成形品が得られる。その際の第3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3図で示す成形品に例えば第6図に示す
ような従来公知のヨーク16と着磁コイル17を
主体とする着磁器を用いて、第3図における左側
の中段のS極(終磁極)に着磁器のN極(起磁
極)付与部を対応させ、右側の中段のN極に着磁
器のS極付与部を対応させて、十分に強い電流を
付与しつつ着磁を行なえば成形品のS極とN極が
反転し、第5図下段に示すように成形品周面にお
いてS極とN極が交互に着磁されているマグネツ
トローラーが得られる。すなわち、成形品の一部
の磁極の磁性はそのまま残して利用し、他の磁極
の磁性を反転させて所望の磁極の配置が形成され
る。第5図下段の成形品の表面磁束密度の分布は
第4図に示す様になつている。
以上のような方法で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。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象ローラーとして
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14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 method for manufacturing a magnet roller, which is a resin magnet used in a magnetic brush developing roller used in a copying machine, a printer, etc., and a mold that can be used therein. [Prior art] Magnetic 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.
In addition, in recent years, the injection molding method has been used to
-28287 and Japanese Patent Publication No. 56-108207, which has integrated polar anisotropic orientation molding inside.
A large number of applications have been filed. 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. Regarding polar anisotropic orientation, methods have been proposed in which a coil is placed inside or outside the mold, or a permanent magnet is placed, but these methods have the following practical problems. A method in which a coil that generates a pulsed magnetic field is built into the mold is ideal because the device is small, but because the pulse width is short, the degree of orientation does not improve and high performance cannot be obtained. . In particular, magnetic rollers for electrostatic phenomena require a high surface magnetic flux density, so a molding material with a high content of magnetic powder is used, so the apparent viscosity of the molding material is extremely high, and it must be oriented using a pulsed magnetic field. In reality, this would have been almost impossible. The method of incorporating a permanent magnet inside the mold is effective because it is relatively small in terms of equipment, but since the viscosity of the molding material is high in the magnetic roller, it is difficult to completely orient the magnetic powder. I couldn't let it go. In addition, during mass production, the molded product is strongly attracted to the mold, so if the cycle is not extended until it is completely cooled when it is released from the mold, warping and other deformations will occur, resulting in a very low yield. In terms of mass production, there were problems due to inefficiency. Regarding the method in which a coil that generates a static magnetic field is built into a mold, if the number of poles is more than two and the polar orientation is anisotropic, the arrangement of the magnetic poles in the mold can be arranged in various directions as shown in Figure 9. Since the cavities cannot be lined up on the partying line, the space required around the cavities becomes large, and a large space is also required to house the coil. In addition, the number of pieces to be produced was limited, resulting in very low productivity in mass production. When installing a coil that generates a static magnetic field outside the mold, if the magnet has more poles than a two-pole magnet and is oriented anisotropically, the magnetic pole arrangement near the cavity will be the same as above, resulting in the same problem. In addition to this, the magnetic path for connecting to the coil outside the mold spreads inside and outside the mold, so there is the problem that the space required to form one cavity becomes larger than with the internal mold type. It was hot. Therefore, since it is very difficult to produce a large number of pieces, it has the disadvantage that productivity is very poor. Furthermore, in terms of the performance of the magnetic roller, if the number of poles is greater than 4, the degree of orientation will decrease, which is a drawback of polar anisotropic orientation, and the oriented portion will only be near the surface layer.
The disadvantage is that magnetic efficiency decreases because the magnetic powder near the center is not effectively utilized. This is due to the following two major theoretical drawbacks. a○ As shown in Figure 12, as the number of poles increases, the shortest distance between adjacent magnetic pole pairs, which forms a magnetic circuit which is the principle of polar anisotropic orientation, becomes the chord connecting them over the shortest distance. The more the number of poles increases, the more the part where the magnetic field is strongly applied moves toward the outer surface relative to the center of the cavity. For this reason, in the center, there is a very weak leakage defined by the permeance between the gaps of the magnetic poles, and orientation can only be achieved by magnetic flux. Since the apparent clay content was very high, the magnetic powder could not be perfectly oriented, resulting in a decrease in properties. b○ As the number of magnetic poles further increases, the pairs of magnetic poles are no longer placed facing each other, so the lines of magnetic force do not pass through the gap in the cavity between the magnetic poles, which forms an adjacent magnetic circuit, and instead flow as shown by the arrow in Figure 13. However, there is a drawback that leakage occurs directly between the magnetic poles around the cavity. For this reason, the efficiency of the magnetic circuit within the mold has been greatly reduced. As a result, there was a drawback that the degree of orientation was lowered and the properties were lowered. Furthermore, as a method of manufacturing rotors for motors rather than for electrostatic phenomena, a method was developed in which two poles are molded and oriented in one direction, and multiple poles are used for magnetization.
38159 and Japanese Patent Application Laid-open No. 112310/1983.
It is not stated that these can solve the problem of the magnetic poles spreading in multiple directions within the mold, but it can be easily inferred by analogy. However, these conventional methods have had the following problems when producing a magnetic roller for electrostatic phenomena. (A) Magnetism is weak. In the case of polar anisotropic orientation, in order to effectively use most of the volume of the magnetic roller, it is possible to increase the degree of orientation with good magnetic efficiency even in the mold, unless the magnetic roller is particularly multipole. However, in the case of two-pole orientation multipolar magnetization, since orientation is performed using a uniformly parallel magnetic field as shown in FIG. 10, the molded product becomes as shown in FIG. 11. 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. When magnetizing, the deviated part is not a magnetic path, so the vector shifts 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 it is considerably inferior to polar anisotropic orientation. (B) Distribution characteristics cannot be controlled. In addition to the above-mentioned high surface magnetic flux density, the required characteristics of a magnetic roller for electrostatic phenomena include:
What particularly affects the image characteristics is the quality of the distribution of the magnetic flux emitted into space from the magnetic roller. Although polar anisotropic orientation has no problems in this respect, it has been found that bipolar orientation and multipolar magnetized rollers have various drawbacks. In other words, as a magnetic roller, it is necessary to have uniform and straight spikes of toner in the phenomenon area, and it is also necessary to suddenly increase the surface magnetic flux density locally in the circumferential direction distribution. It is necessary by design to lower or lower it.
However, in the method of performing bipolar oriented multipole magnetization, the anisotropy direction of the magnetic powder is oriented in a single direction at the required magnetic pole position on the magnet roller, as described above. The surface magnetic flux density waveform also has a distribution uniquely determined by the magnetic powder oriented in a single direction because it is not focused to the required waveform. It was extremely difficult to control the magnet simply by changing the shape of the yoke and the strength of magnetization. Moreover, it was impossible to perform full-power magnetization and control the distribution waveform at the same time in order to increase the absolute value of the surface magnetic flux density. In other words, in a magnetic roller that applies polar anisotropic orientation, it is possible to simultaneously satisfy the surface magnetic flux density distribution and height when the number of poles is small, but industrial productivity is extremely low. There are drawbacks, such as the fact that although the productivity is high, it is impossible to produce a magnetic roller that uses two-pole oriented multi-pole magnetization, but has a high surface magnetic flux density and clear distribution characteristics. The present invention has been made in view of the above-mentioned problems, and its purpose is to make it possible to obtain strong magnetic force even with a high content of magnetic powder by oriented with a high degree of orientation, and to obtain a strong magnetic force with a high surface magnetic flux density. It is an object of the present invention to provide a method for manufacturing a magnetic roller, which can control the thickness and distribution, has a good yield, can be manufactured in large numbers, and has good productivity, and a mold that can be used therein. [Means for Solving the Problems] The above object of the present invention is to provide a plurality of magnetic pole pairs constituting three or more of magnetic pole pairs consisting of a pair of opposing magnetomotive poles and a magnetization pole in the peripheral part in a cross section perpendicular to the axis. has magnetic poles, and the magnetic poles are arranged so 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 , magnetic powder 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 in the central part of the cross section connects the magnetizing pole and the final magnetizing pole of each pair of magnetic poles. A method for manufacturing a magnetic roller oriented substantially parallel to a straight line, comprising: a. A plurality of orienting magnetic pole pairs consisting of a magnetizing pole and a magnetizing pole being oriented on one side with a roller molding cavity in between. The magnetic poles are arranged so that the final magnetic pole is lined up on the other side and correspond to the arrangement of the magnetic pole pairs of the magnetic roller, and magnetic fluxes in the same direction and substantially parallel to each other are applied to the cavity from these orienting magnetic pole pairs. A resin material containing the injected magnetic powder is molded to have magnetic poles at positions corresponding to the respective orientation magnetic poles, and the magnetic powder is directed toward the center of the magnetic peak of each orientation magnetic pole in the vicinity of each orientation magnetic pole. a step of obtaining a roller-shaped molded product that is oriented substantially parallel in a direction in which the magnetic fluxes are converged, and which are otherwise substantially parallel to each other in response to the substantially parallel magnetic flux generated from each pair of magnetic poles; b. the roller obtained in step a; This is achieved by a method for manufacturing a magnetic roller, which comprises the steps of reversing the magnetism of a part of the magnetic poles of a shaped molded product and magnetizing adjacent magnetic poles so that they are different. Moreover, the mold of the present invention that can be used in the above step a,
In order to mold a magnet roller in which a resin material containing magnetic powder is molded and oriented, a magnetomotive pole member for orientation and a final magnetization pole member for orientation are respectively provided on the left and right sides of a line passing through the center of the cross section of a cavity made of a magnetic material, and each of the above-mentioned In order to divide the magnetic pole member into at least three parts, a spacer made of a non-magnetic pole material having a longitudinal shape parallel to the center line is provided so that the longitudinal direction of each spacer is parallel to the center line of the cavity cross section, and
The tip of each spacer is arranged so as to constitute a part of the cavity, and the lines of magnetic force from the magnetomotive pole member are divided by the spacer and the magnetic powder in the cavity is divided into the magnetomotive pole and the final magnetization pole. The magnetic poles are arranged to be substantially parallel to each other in the cross section along a straight line connecting the magnetic poles, and to converge toward the center of the magnetic peak of each magnetic pole. In the method of the present invention, conventionally known resin magnet materials (ferromagnetic powder and binder) are used, but the orienting force is applied by flowing magnetic lines of force in one direction to the molded product during molding orientation. Since it is large and all of the magnetic powder in the center of the magnet roller is oriented, materials with a high content of ferromagnetic powder can be used without difficulty. In the present invention, the surface magnetic flux density of the molded product is improved by changing the material of the ferromagnetic material forming the magnetic poles for applying the magnetic lines of force for orientation, by changing the cross-sectional area of the magnetic poles, or by changing both. can be easily controlled. In other words, by changing the amount of magnetic flux passing between each magnetic pole using the method described above, and changing the volume ratio of the magnetic powder oriented due to the magnetic chain occurring at each pole inside the molded product, the surface magnetic flux density can be increased. This means that the distribution can be controlled without changing the strength of magnetization, with each pole fully magnetized, and the maximum energy of all the magnetic powder inside the magnet roller can be extracted. Hereinafter, the present invention will be specifically described with reference to the drawings. [Example] FIGS. 1 to 6 schematically show each process of an example of the present invention. Further, FIGS. 9 to 11 show conventional embodiments. Figure 1 is a drawing of the cavity in the mold that best represents the features of the present invention. In the figure, 1 and 4 are for orientation of magnetic powder made of ferromagnetic materials facing each other with the cavity in between. This is a magnetic pole (magnetic pole member) for guiding the magnetic flux from the magnetic field generating coils shown at 24 and 18 in the molding machine shown in FIG. 8 through the molding machine platen shown at 25 and 20 to the mold cavity. . Furthermore, 7, 8, 9 and 10, 11, 12 are
This is a magnetic pole portion that is integrally constructed with the magnetic poles 1 and 4 above, and is arranged to substantially face each other across a cylindrical cavity space indicated by 14. That is, magnetic pole parts 7, 8, and 9, which serve as magnetomotive poles through which lines of magnetic force flow, and magnetic pole parts 10, 11, and 12, which serve as final magnetic poles into which lines of magnetic force flow, are lined up facing each other. and 12 each form a pair of magnetic poles, and a line connecting 7 and 10,
Each magnetic pole part is arranged so that the line connecting 8 and 11 and the line connecting 9 and 12 are substantially on the same plane and are substantially parallel. Here, each magnetic pole is constructed of a ferromagnetic material as is conventionally known. Also 2, 3, 5,
6 is a spacer made of a non-magnetic material. That is, the mold of the molding machine shown in FIG. 8 is characterized by having a pair of magnetic poles 1 and 4 facing each other with the cavity in between, and having a magnetic pole part separated by a spacer made of a non-magnetic material at the end on the cavity side. There is. By having such a configuration in the mold, it becomes possible to distribute and arrange the magnetic pole parts on both sides of the parting part in the molding machine, creating extra space along the parting surface in the molding machine, and making it possible to By using this method, a large number of cavities can be parallelized to enable multi-cavity production. In such a configuration, 18,
When a current is applied to the magnetic field generating coil 24, the magnetic flux (magnetic field lines) generated there passes through the movable molding machine platen 20, and is transferred from the magnetic pole 1 made of the ferromagnetic material in the mold to the magnetic flux 2, It is divided into 8 and 9 magnetic pole parts (magnetic poles), flows into 14 cavities, and flows according to the permeance distribution between the gaps as shown at 13 in Figure 1, and the opposing 10, 11, 1
The current flows to gather at the second magnetic pole (final magnetic pole). The magnetic flux passes through the magnetic pole 4, the fixed platen shown at 25 in FIG. 8, and the tie bar shown at 19.
It is configured to be 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, the magnetic flux shown in Fig. 2 is obtained. The orientation of the powder 15 occurs according to the flow of magnetic field lines shown in FIG. As shown in Figure 1, the lines of magnetic force spread inside the cavity and converge at the magnetic pole, so
The magnetic powder is also oriented in a converged state at the magnetic pole portion, as shown in FIG. 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. 2, and taken out, a molded article shown in FIG. 3 is obtained. At this time, the distribution of surface magnetic flux density of the molded product shown in FIG. 3 becomes as shown in the upper part of FIG. 5. Next, using a conventionally known magnetizer mainly consisting of a yoke 16 and a magnetizing coil 17 as shown in FIG. 6, the molded product shown in FIG. If you match the N-pole (magnetizing pole) applying part of the magnetizer to the magnetic pole (magnetic pole) and the S-pole applying part of the magnetizer to the middle N pole on the right side, magnetize while applying a sufficiently strong current. The S and N poles of the molded product are reversed, and a magnetic roller is obtained in which the S and N poles are alternately magnetized on the peripheral surface of the molded product, as shown in the lower part of FIG. That is, the magnetism of some of the magnetic poles of the molded product is left intact and used, and the magnetism of other magnetic poles is reversed to form a desired magnetic pole arrangement. The surface magnetic flux density distribution of the molded product shown in the lower row of FIG. 5 is as shown in FIG. 4. Four-pole and six-pole plastic magnet rollers were created using the method described above and evaluated. The evaluation is compared with the typical specifications generally required for a copying machine roller, which has a maximum surface magnetic flux density of 900 [G] or more and a width at half-life of 60% or less. Note that the half-life time width is expressed by the following formula using A and B shown in FIG. 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】
以上説明したように、本発明のマグネツトロー
ラーの製造方法によれば、
金型内磁極部の全てがほぼ同一方向に向いた対
向した磁極構造をとるため、パーテイング面に添
つて空間の余裕ができて多数個取りが容易であ
り、生産性を3〜6倍にもすることができる。
また、磁力の必要な所へ配向用磁束が収束され
て磁性粉の磁化容易軸(磁力線に添うように向く
磁性粉の中心軸のこと)のベクトルが収束される
ため、表面磁束密度の特性について大幅な性能向
上が達成される。
また、脱磁工程が必要ないため、脱磁用装置が
不必要で生産性が良い。
また磁極部間を通過する磁束量を磁極部対間で
変化させて使用される磁性粉の体積比率を変化さ
せれば、フル着磁での状態で表面着磁密度の分布
のコントロールを行なうことが可能である。
As explained above, according to the method for manufacturing a magnetic roller of the present invention, all of the magnetic pole parts in the mold have a magnetic pole structure in which they face each other in substantially the same direction, so that there is sufficient space along the parting surface. It is easy to produce a large number of pieces, and productivity can be increased by 3 to 6 times. In addition, since the orientation magnetic flux is focused where the magnetic force is needed, and the vector of the easy axis of magnetization of the magnetic powder (the central axis of the magnetic powder that is oriented along the lines of magnetic force) is focused, the characteristics of the surface magnetic flux density are Significant performance improvements are achieved. In addition, since a demagnetizing process is not required, a demagnetizing device is not required, resulting in good productivity. In addition, by changing the amount of magnetic flux passing between the magnetic pole parts and changing the volume ratio of the magnetic powder used, it is possible to control the distribution of surface magnetization density in a fully magnetized state. is possible.
第1図は本発明の金型のキヤビテイー近傍の断
面図、第2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3図は、成形取
り出し後のマグネツトローラーの断面図、第4図
は着磁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の磁束分布を、
下段は着磁後の磁束分布をそれぞれ示す)、第6
図は着磁器の模式図、第7図は第2図と同様で4
極のもの、第8図は本実施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図は従来から
の極異方性配向成形による配向方法を示す模式
図、第10図は2極配向を説明する模式図、第1
1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12図は極異方性配向品の
断面図、第13図は従来からの極異方性配向成形
による配向方法の問題点を示す模式図、第14図
は半減時幅を説明する図、第15図はマグネツト
ローラーを現像機に装着している部分の模式図で
ある。
1,4…磁極(磁極部材)(なお、1は起磁極
部材、4は終磁極部材である。)、2,3,5,6
…スペーサー(非磁性材)、7,8,9…磁極部
(起磁極)、10,11,12…磁極部(終磁極)、
13…磁束(磁力線)の流れ、14…金型内キヤ
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、2
0…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 vicinity of the cavity of the mold of the present invention, Fig. 2 is a sectional view of the resin magnet material injected and oriented into the cavity, and Fig. 3 is a sectional view of the magnet roller after being removed from the mold. , Fig. 4 is a cross-sectional view of the magnet roller after magnetization, Fig. 5 is a magnetic flux distribution graph on the circumferential surface of the magnet roller (the upper part of Fig. 5 shows the magnetic flux distribution after molding,
The lower row shows the magnetic flux distribution after magnetization), the sixth
The figure is a schematic diagram of the magnetizer, and Figure 7 is the same as Figure 2.
FIG. 8 is a schematic diagram showing the magnetic field injection molding apparatus and mold part used in this example, FIG. 9 is a schematic diagram showing the orientation method using conventional polar anisotropic orientation molding, and FIG. The figure is a schematic diagram explaining bipolar orientation.
Figure 1 is a cross-sectional view of a magnetic roller obtained by demagnetizing and re-magnetizing a bipolar oriented product, Figure 12 is a cross-sectional view of a polar anisotropically oriented product, and Figure 13 is a cross-sectional view of a magnetic roller produced by conventional polar anisotropically oriented molding. FIG. 14 is a diagram illustrating the half-width, and FIG. 15 is a schematic diagram showing the part where the magnetic roller is attached to the developing machine. 1, 4...Magnetic pole (magnetic pole member) (1 is the magnetizing pole member, 4 is the final magnetizing pole member), 2, 3, 5, 6
... Spacer (non-magnetic material), 7, 8, 9... Magnetic pole part (magnetic pole), 10, 11, 12... Magnetic pole part (final magnetic pole),
13...Flow of magnetic flux (lines of magnetic force), 14...Mold cavity, 15...Magnetic powder, 16...Yoke, 17...
Magnetizing coil, 18, 24... Magnetic field generation coil, 2
0...Movable side molding machine platen, 21...Fixed side mold,
23... Movable side mold, 25... Fixed side molding machine platen, 26, 27, 28... Magnetic pole.
Claims (1)
向する一対の起磁極と終磁極とからなる磁極対の
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、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 起磁極と終磁極からなる配向用磁極対の複数
を、ローラー成形用キヤビテイーを挟んで一方
の側に起磁極が、他方の側に終磁極が並び、か
つ前記マグネツトローラーの磁極対の配置に対
応するように配置し、これら配向用磁極対から
同一方向の互いにほぼ平行な磁束をかけつつ該
キヤビテイーに注入された磁性粉を含む樹脂材
料を成形し、各配向用磁極に対応する位置に磁
極を有し、かつ前記磁性粉が各配向用磁極近傍
において各配向用磁極の磁気的ピークの中心に
向つて収束する方向で、それ以外の部分では各
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、 b 該工程aで得られたローラー状成形品の磁極
の一部の磁性を反転させ、隣りあう磁極が異な
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。 2 磁性粉を含む樹脂材料を成形配向したマグネ
ツトローラーを成形するために磁性材で作つたキ
ヤビテイーの断面中心を通る線上の左右にそれぞ
れ配向用起磁極部材と配向用終磁極部材を設け、 前記各磁極部材を少なくとも3分割するため
に、前記中心線に平行な長手形状の非磁極材で作
つたスペーサーを前記キヤビテイー断面中心線と
各スペーサーの長手方向が平行であつて、かつ、
前記各スペーサーの先端部がキヤビテイーの一部
を構成するように配置し、 前記起磁極部材からの磁力線は前記スペーサー
によつて分割されてキヤビテイー内の前記磁性粉
を、前記起磁極と前記終磁極を結ぶ直線上に沿つ
て前記断面において互いにほぼ平行となり、か
つ、各磁極の磁気的ピークの中心に向つて収束す
るように構成したことを特徴とするマグネツトロ
ーラー成形用金型。[Scope of Claims] 1. A plurality of magnetic poles constituting three or more of magnetic pole pairs consisting of a pair of opposing magnetomotive poles and a magnetization pole, are provided in a peripheral portion in a cross section perpendicular to the axis, and the magnetic poles are , straight lines connecting the magnetizing pole and the final magnetizing pole in each pair of magnetic poles are arranged so that they are substantially parallel to each other on the cross section, and adjacent magnetic poles have different magnetisms; It is oriented in a direction that converges toward the center of the magnetic peak of each magnetic pole in the peripheral part, and in the central part of the cross section, it is almost parallel to a straight line connecting the magnetizing pole and the final magnetizing pole of each pair of magnetic poles. A method for manufacturing an oriented magnetic roller, comprising: a. A plurality of pairs of orienting magnetic poles each consisting of a magnetomotive pole and a final magnetization pole, with the magnetomotive pole on one side and the final magnetization pole on the other side with a roller molding cavity in between. A resin containing magnetic powder, which is arranged so that the magnetic poles are aligned and corresponds to the arrangement of the magnetic pole pairs of the magnetic roller, and is injected into the cavity while applying magnetic flux in the same direction and substantially parallel to each other from the orienting magnetic pole pairs. Molding a material, having a magnetic pole at a position corresponding to each orientation magnetic pole, and in a direction in which the magnetic powder converges toward the center of the magnetic peak of each orientation magnetic pole in the vicinity of each orientation magnetic pole; The part includes a step of obtaining a roller-shaped molded product that is oriented substantially parallel in response to the nearly parallel magnetic flux generated from each pair of magnetic poles, and (b) a part of the magnetic pole of the roller-shaped molded product obtained in step a. 1. A method for manufacturing a magnetic roller, comprising the step of reversing the magnetism of the magnetic roller and magnetizing adjacent magnetic poles so that they are different from each other. 2. In order to mold a magnet roller in which a resin material containing magnetic powder is molded and oriented, a magnetizing pole member for orientation and a final magnetizing pole member for orientation are respectively provided on the left and right sides of a line passing through the center of the cross section of a cavity made of a magnetic material, and the above-mentioned. In order to divide each magnetic pole member into at least three parts, a spacer made of a non-magnetic pole material having a longitudinal shape parallel to the center line is provided so that the longitudinal direction of each spacer is parallel to the center line of the cavity cross section, and
The tip of each spacer is arranged so as to constitute a part of the cavity, and the lines of magnetic force from the magnetomotive pole member are divided by the spacer and the magnetic powder in the cavity is divided into the magnetomotive pole and the final magnetization pole. A mold for molding a magnetic roller, characterized in that the cross section is substantially parallel to each other along a straight line connecting the magnetic poles, and converges toward the center of the magnetic peak of each magnetic pole.
Priority Applications (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2558487A JPS6464208A (en) | 1987-02-07 | 1987-02-07 | Manufacture of 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 |
|---|---|---|---|
| JP2558487A JPS6464208A (en) | 1987-02-07 | 1987-02-07 | Manufacture of magnet roller |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6464208A JPS6464208A (en) | 1989-03-10 |
| JPH0533802B2 true JPH0533802B2 (en) | 1993-05-20 |
Family
ID=12169964
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2558487A Granted JPS6464208A (en) | 1986-05-20 | 1987-02-07 | Manufacture of magnet roller |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6464208A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP5722944B2 (en) * | 2013-04-26 | 2015-05-27 | 株式会社日本製鋼所 | Manufacturing method of plastic magnet |
Family Cites Families (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS60124812A (en) * | 1983-12-09 | 1985-07-03 | Seiko Epson Corp | Manufacture of permanent magnet |
| JPH0126418Y2 (en) * | 1984-09-20 | 1989-08-08 | ||
| JPS61112310A (en) * | 1984-11-07 | 1986-05-30 | Sumitomo Bakelite Co Ltd | Manufacture of permanent magnet |
-
1987
- 1987-02-07 JP JP2558487A patent/JPS6464208A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6464208A (en) | 1989-03-10 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| LAPS | Cancellation because of no payment of annual fees |