JPH04139706A - Magnet roll and manufacture thereof - Google Patents
Magnet roll and manufacture thereofInfo
- Publication number
- JPH04139706A JPH04139706A JP26203090A JP26203090A JPH04139706A JP H04139706 A JPH04139706 A JP H04139706A JP 26203090 A JP26203090 A JP 26203090A JP 26203090 A JP26203090 A JP 26203090A JP H04139706 A JPH04139706 A JP H04139706A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- magnetic field
- main pole
- pole
- magnet roll
- 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.)
- Granted
Links
- 238000004519 manufacturing process Methods 0.000 title claims description 13
- 230000005291 magnetic effect Effects 0.000 claims abstract description 115
- 238000009826 distribution Methods 0.000 claims abstract description 14
- 238000000034 method Methods 0.000 claims description 11
- 238000000465 moulding Methods 0.000 claims description 7
- 239000000126 substance Substances 0.000 abstract description 4
- 230000005389 magnetism Effects 0.000 abstract 4
- 230000005294 ferromagnetic effect Effects 0.000 abstract 1
- 239000011347 resin Substances 0.000 description 5
- 229920005989 resin Polymers 0.000 description 5
- 238000001125 extrusion Methods 0.000 description 4
- 230000004907 flux Effects 0.000 description 4
- 239000000696 magnetic material Substances 0.000 description 4
- 238000012805 post-processing Methods 0.000 description 4
- 239000000853 adhesive Substances 0.000 description 3
- 230000001070 adhesive effect Effects 0.000 description 3
- BZHJMEDXRYGGRV-UHFFFAOYSA-N Vinyl chloride Chemical compound ClC=C BZHJMEDXRYGGRV-UHFFFAOYSA-N 0.000 description 2
- 238000004140 cleaning Methods 0.000 description 2
- 230000000052 comparative effect Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000005284 excitation Effects 0.000 description 2
- -1 polyethylene Polymers 0.000 description 2
- 229910000859 α-Fe Inorganic materials 0.000 description 2
- 229920000178 Acrylic resin Polymers 0.000 description 1
- 239000004925 Acrylic resin Substances 0.000 description 1
- 239000004709 Chlorinated polyethylene Substances 0.000 description 1
- 239000004952 Polyamide Substances 0.000 description 1
- 239000004698 Polyethylene Substances 0.000 description 1
- 239000004734 Polyphenylene sulfide Substances 0.000 description 1
- 239000004743 Polypropylene Substances 0.000 description 1
- QJVKUMXDEUEQLH-UHFFFAOYSA-N [B].[Fe].[Nd] Chemical compound [B].[Fe].[Nd] QJVKUMXDEUEQLH-UHFFFAOYSA-N 0.000 description 1
- 229910045601 alloy Inorganic materials 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- KPLQYGBQNPPQGA-UHFFFAOYSA-N cobalt samarium Chemical compound [Co].[Sm] KPLQYGBQNPPQGA-UHFFFAOYSA-N 0.000 description 1
- 238000000748 compression moulding Methods 0.000 description 1
- UQLDLKMNUJERMK-UHFFFAOYSA-L di(octadecanoyloxy)lead Chemical compound [Pb+2].CCCCCCCCCCCCCCCCCC([O-])=O.CCCCCCCCCCCCCCCCCC([O-])=O UQLDLKMNUJERMK-UHFFFAOYSA-L 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 239000003302 ferromagnetic material Substances 0.000 description 1
- 238000009472 formulation Methods 0.000 description 1
- 230000001771 impaired effect Effects 0.000 description 1
- 238000001746 injection moulding Methods 0.000 description 1
- 239000006249 magnetic particle Substances 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 239000000113 methacrylic resin Substances 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- 230000005405 multipole Effects 0.000 description 1
- 229910001172 neodymium magnet Inorganic materials 0.000 description 1
- 239000008188 pellet Substances 0.000 description 1
- 230000002093 peripheral effect Effects 0.000 description 1
- 229920002647 polyamide Polymers 0.000 description 1
- 229920000515 polycarbonate Polymers 0.000 description 1
- 239000004417 polycarbonate Substances 0.000 description 1
- 229920000728 polyester Polymers 0.000 description 1
- 229920000573 polyethylene Polymers 0.000 description 1
- 229920000069 polyphenylene sulfide Polymers 0.000 description 1
- 229920001155 polypropylene Polymers 0.000 description 1
- 239000000843 powder Substances 0.000 description 1
- 229910000938 samarium–cobalt magnet Inorganic materials 0.000 description 1
- 239000000057 synthetic resin Substances 0.000 description 1
- 229920003002 synthetic resin Polymers 0.000 description 1
- LENZDBCJOHFCAS-UHFFFAOYSA-N tris Chemical compound OCC(N)(CO)CO LENZDBCJOHFCAS-UHFFFAOYSA-N 0.000 description 1
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は電子複写機やレーザープリンター等における現
像装置やクリーニング装置に用いられるマグネットロー
ルとその製造方法に関し、更に詳しくは良質なコピー画
質の得られる一体成形マグネットロールとその製造方法
に関するものである。[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a magnetic roll used in a developing device or a cleaning device in an electronic copying machine, a laser printer, etc., and a method for manufacturing the same, and more specifically relates to a method for producing a magnetic roll used in a developing device or a cleaning device in an electronic copying machine or a laser printer. The present invention relates to an integrally molded magnet roll and a manufacturing method thereof.
従来のマグネットロールには第7図に示す如く複数のマ
グネットをシャフトに沿って貼り合わせた接着型と、一
体成形されたマグネットロール表面に、磁性粒子の配向
方向が磁極表面に集束するような配向方式、即ち極異方
配向方式を用いて複数の磁極を着磁させて作成した多極
一体型とがある。Conventional magnet rolls include an adhesive type in which multiple magnets are bonded together along a shaft, as shown in Figure 7, and an adhesive type in which a plurality of magnets are bonded together along a shaft, and an oriented type in which the orientation direction of magnetic particles is focused on the magnetic pole surface on the surface of the integrally molded magnet roll. There is a multi-pole integrated type, which is created by magnetizing a plurality of magnetic poles using a polar anisotropic orientation method.
ところで、良好なコピー画質を得る為には、マグネット
ロール全体のラジアル磁界成分の周方向分布図において
少なくとも1つの極の磁界パタンかそのピーク位置をは
さんで左右非対称となっていることが必要である。By the way, in order to obtain good copy image quality, it is necessary that the magnetic field pattern of at least one pole or its peak position be asymmetrical in the circumferential direction distribution diagram of the radial magnetic field component of the entire magnet roll. be.
接着型のものは貼り合わす各マグネットを個別に着磁さ
せることができる為、磁界パタンの自由度が高く、左右
非対称な磁界パタンを得ることが容易であり、従って高
性能マグネットロールの製法に適している。しかしその
反面、複数の長尺マグネットを全長にわたって高精度に
貼り合わせるのは困難であり、製造コストが高くなると
いう問題がある。一方、極異方配向型は貼り合わせが不
要なので製造コストが下げられるという長所があること
から、例えば特開昭56−108207号等、近年盛ん
に研究されているものの、従来の極異方配向型ではそれ
を成形する金型の磁気回路の事情から、各磁極の周方向
磁界パタンはそのピークを挟んでほとんど左右対称にな
ってしまい非対称パタンか得られないという問題があっ
た。さらに詳しくいえば磁界パタンの底部(磁界パタン
のベースライン付近)は非対称になり得るものの、ピー
ク値存在位置から磁界強度がピーク値の1/2となる範
囲内の領域においては、その磁界パタンか非対称になる
ということはな(、コピー画質の劣るマグネットロール
しか得られないのが現状であった。The adhesive type allows each magnet to be bonded to be individually magnetized, so there is a high degree of freedom in the magnetic field pattern, and it is easy to obtain an asymmetrical magnetic field pattern, making it suitable for manufacturing high-performance magnetic rolls. ing. However, on the other hand, it is difficult to bond a plurality of elongated magnets together over their entire lengths with high precision, resulting in an increase in manufacturing costs. On the other hand, the extremely anisotropically oriented type has the advantage of reducing manufacturing costs because it does not require bonding. Due to the magnetic circuit of the mold used to mold the mold, the circumferential magnetic field pattern of each magnetic pole becomes almost symmetrical with respect to its peak, making it impossible to obtain an asymmetrical pattern. More specifically, although the bottom of the magnetic field pattern (near the baseline of the magnetic field pattern) can be asymmetrical, in the region where the magnetic field strength is 1/2 of the peak value from the peak value position, the magnetic field pattern (Currently, only magnetic rolls with inferior copy quality could be obtained.
これを解決する手段として、マグネットロール表面に長
手方向に凹部、凸部あるいは7字溝等を設けて磁界パタ
ンの対称性をくずす方法が開示されている(特開昭63
−5371 、特開昭63−7604)。As a means to solve this problem, a method has been disclosed in which the symmetry of the magnetic field pattern is disrupted by providing recesses, protrusions, or 7-shaped grooves in the longitudinal direction on the surface of the magnet roll (Japanese Patent Application Laid-Open No. 63-11111).
-5371, JP-A-63-7604).
しかし凹部、凸部、7字溝等を後加工で設けることは、
コスト高を招き、又、凹部、凸部、7字溝を形成せしめ
るための構造を有する金型を用いてマグネットロールを
成形すれば後加工は不要になるものの、金型やダイの最
適設計と製作に多大の時間を要し、しかも金型の摩耗に
より磁気パターンが変化するという問題点もある。However, it is not possible to provide recesses, protrusions, 7-shaped grooves, etc. in post-processing.
In addition, if the magnet roll is formed using a mold that has a structure for forming concave portions, convex portions, and 7-shaped grooves, post-processing will be unnecessary, but it will not be possible to optimize the design of the mold or die. Another problem is that it takes a lot of time to manufacture, and the magnetic pattern changes due to wear of the mold.
本発明はかかる現況に鑑みて成されたものであり、一体
成形によって得ることができ、しかもマグネットロール
表面に凹部、凸部、7字溝等を設けなくても非対称磁界
パタンか得られる極異万−体型マグネットロールを提供
することを目的とするもので、後加工の必要がないとと
もに複雑な金型を用いる必要もなく、又、金型が摩耗し
ても安定した磁気パタンを有し、良好なコピー画質をも
たらすことができるマグネットロールを提供せんとする
ものである。The present invention has been made in view of the current situation, and is extremely unique in that an asymmetrical magnetic field pattern can be obtained by integral molding and even without providing recesses, protrusions, 7-shaped grooves, etc. on the surface of the magnet roll. The purpose is to provide a universal magnetic roll that does not require post-processing, does not require the use of complicated molds, and has a stable magnetic pattern even if the mold wears out. It is an object of the present invention to provide a magnetic roll that can provide good copy image quality.
本発明者らは上記問題を解決するためには、極異方磁場
配向法にてマグネットロールを成形する際に用いる金型
の構造を、第2図に示すように、磁界発生のための複数
個のヨークのうち非対称磁界パタンを形成すべきマグネ
ットロール磁極に対応するヨークの先端幅と該ヨークに
隣接するヨークの先端幅とが異なる値を持つ構造とすれ
ば、凹部、凸部、7字溝等を設けな(でも、非対称磁界
パタンを有する一体成形型マグネットロールを作り得る
ことを見出している。しかしながら、この方法では幅広
のヨークに対応するマグネットロール磁極、即ち、非対
称化すべき磁極に隣接する磁極が発する磁界パタンか必
然的に幅広くなって、ピーク値も低(なる為に、マグネ
ットロールが必要とする多様な要求性能を満たし得ない
場合が生じる。In order to solve the above problem, the present inventors developed a structure of a mold used when forming a magnet roll using the polar anisotropic magnetic field orientation method, as shown in Figure 2. Among the yokes, if the structure is such that the tip width of the yoke corresponding to the magnet roll magnetic pole that is to form an asymmetrical magnetic field pattern has a different value from the tip width of the yoke adjacent to the yoke, there are concave portions, convex portions, It has been found that it is possible to produce an integrally molded magnet roll with an asymmetrical magnetic field pattern without providing grooves, etc. However, in this method, the magnetic roll magnetic pole corresponding to the wide yoke, i.e. The magnetic field pattern generated by the magnetic poles inevitably becomes wider and the peak value becomes low (as a result, there are cases where the magnetic roll cannot meet the various required performances.
本発明者らはかかる問題を解決するため鋭意研究した結
果、非対称パタンとすべき磁極(以下、主極と呼ぶこと
にする)に隣接する2つの磁極のうち主極のパタンか急
峻となる側に位置する磁極(以下、第1隣接極と呼ぶ、
他のもう1つの隣接極を第2隣接極と呼ぶことにする)
を形成する為の導磁路が、その先端近傍に、隣接する導
磁路に向かう突出部を有する構造となせばよいことを見
出して本発明に到達したのである。該導磁路の突出部形
状は目的とする非対称性や磁極の磁場強度に応じて設計
すればよく、又、第1隣接極形成用導磁路に於て突出部
の突出方向は、主極形成用導磁路に向かわしめることも
、又、主極形成用導磁路とは反対側に位置する導磁路に
向かわしめることも可能である。As a result of intensive research to solve this problem, the present inventors found that of the two magnetic poles adjacent to the magnetic pole (hereinafter referred to as the main pole) that should have an asymmetric pattern, the side where the pattern of the main pole is steeper. (hereinafter referred to as the first adjacent pole,
The other adjacent pole will be referred to as the second adjacent pole)
The present invention was achieved by discovering that the magnetic guiding path for forming the magnetic guiding path may have a structure in which a protrusion toward the adjacent magnetic guiding path is provided near the tip thereof. The shape of the protruding part of the magnetic guiding path may be designed according to the desired asymmetry and the magnetic field strength of the magnetic pole, and the protruding direction of the protruding part in the first adjacent pole forming magnetic guiding path is It is also possible to direct it to the magnetic guiding path for forming the main pole, or to the magnetic guiding path located on the opposite side to the magnetic guiding path for forming the main pole.
そしてこのような方法により作成されるマグネットロー
ルは、ラジアル磁界成分の周方向パタンにおいて主極の
磁界のピーク値からその強度が少なくとも1/2になる
迄の範囲内の分布波形がピーク値を挟んで実質的に非対
称形となり、且つ該主極からそれに隣接する2つの磁極
のうち少なくとも1つの磁極までを含む領域の外周が実
質的に円弧の一部となるように構成される。A magnet roll made by such a method has a distribution waveform in the circumferential pattern of the radial magnetic field component within a range from the peak value of the magnetic field of the main pole until the strength becomes at least 1/2, with the peak value sandwiched between the peak values. The main pole is substantially asymmetrical, and the outer periphery of the region including the main pole and at least one of the two adjacent magnetic poles is substantially a part of a circular arc.
第1隣接極形成用導磁路の先端近傍に突出部を形成した
ことによりマグネットロールの第1隣接極磁界パタンを
過度に幅広(することなく、従ってそのピーク値を下げ
ることなく、主極の磁界パタンを非対称化することがで
き、良好な複写画像を得るのに好適なマグネットロール
が提供できる。By forming the protrusion near the tip of the magnetic conduction path for forming the first adjacent pole, the first adjacent pole magnetic field pattern of the magnet roll is not made excessively wide (therefore, without lowering its peak value), and the main pole is The magnetic field pattern can be made asymmetrical, and a magnet roll suitable for obtaining good copied images can be provided.
このような効果がもたらされるのは次の理由によると推
測される。It is presumed that this effect is produced for the following reasons.
まず、突出部のない先端幅の広いヨークを使うと、その
先端面全体から略均等な磁束が溶融樹脂マグネットに侵
入する為、その磁極部がほぼ均等に配向着磁されてしま
い、その結果幅広い磁界パタンか形成されると考えられ
る。First, if a yoke with a wide tip without a protrusion is used, almost uniform magnetic flux will enter the molten resin magnet from the entire tip surface, and the magnetic poles will be oriented and magnetized almost evenly, resulting in a wide It is thought that a magnetic field pattern is formed.
一方、先端幅は同じでも突出部構造にすると磁束の一部
が溶融樹脂マグネットロールに侵入せず、この張出部を
経由して主極導磁路へ行ってしまう。On the other hand, even if the tip width is the same, if the protrusion structure is used, a part of the magnetic flux will not enter the molten resin magnet roll, but will go to the main pole magnetic conduction path via this protrusion.
そのため樹脂マグネットに侵入する磁束が均等でなくな
り張出部から侵入する磁束は少ない。従って該マグネッ
トの導磁路突出部に面した領域の磁気特性は低くなり、
第1隣接極のパタンを過度に広げることなく、主極パタ
ンを非対称化できる。Therefore, the magnetic flux that enters the resin magnet is not uniform, and the amount of magnetic flux that enters from the overhang is small. Therefore, the magnetic properties of the area facing the magnetic guide path protrusion of the magnet are low,
The main pole pattern can be made asymmetrical without excessively widening the pattern of the first adjacent pole.
次に本発明の詳細を図示した実施例に基づき説明する。 Next, details of the present invention will be explained based on illustrated embodiments.
本発明に用いられる磁性材料粉末としては樹脂磁石成形
が可能なものなら何でもよく、例えば六方晶フェライト
、サマリウム−コバルト系合金ネオジウム−鉄−ボロン
系等の磁性材料が挙げられる。又、合成樹脂としても特
に制限はなく例えば、塩化ビニル、ポリエチレン、塩素
化ポリエチレン、ポリプロピレン、ポリアミド、ポリエ
ステル、ポリカーボネート、ポリフェニレンサルファイ
ド、アクリル樹脂、メタクリル樹脂等が挙げられ、所望
に応じて適宜選択される。The magnetic material powder used in the present invention may be any material that can be molded into a resin magnet, and examples thereof include magnetic materials such as hexagonal ferrite, samarium-cobalt alloy neodymium-iron-boron system, and the like. Further, there are no particular limitations on the synthetic resin, and examples thereof include vinyl chloride, polyethylene, chlorinated polyethylene, polypropylene, polyamide, polyester, polycarbonate, polyphenylene sulfide, acrylic resin, methacrylic resin, etc., and can be appropriately selected according to desire. .
第1図は本発明に用いる成形金型の1実施例を示し、中
心に非磁性体材料製のコア3を有し、該コア3の外にマ
グネットロール成形空間となる空隙部4が形成され、更
に、該空隙部4の外に強磁性体材料製のダイスヨーク部
1が非磁性体材料製の極間部2を間に介在させた状態で
配置されれている。図中1aとして示すものが主極形成
用導磁路であり、図中1bが第1隣接極形成用導磁路、
ICが第2隣接極形成用導磁路である。又、図中5は第
1隣接極形成用導磁路に形成された張出部であり、張出
部5は主極形成用導磁路1aに向かって突出した構成と
されている。張出部は金型の内面側、即ち、導磁路の先
端近傍において隣接する導磁路に向かって突出していれ
ばよ(、例えば、第3図や第4図に示すような形状とす
ることも可能であり、更に第5図として示す如く、張出
部5を主極形成用導磁路1aとは反対側の導磁路である
第2隣接極形成用導磁路1cに向かって突出した構成と
することも可能である。FIG. 1 shows an embodiment of the molding die used in the present invention, which has a core 3 made of a non-magnetic material at the center, and a gap 4 which becomes a magnetic roll molding space is formed outside the core 3. Further, a die yoke portion 1 made of a ferromagnetic material is arranged outside the gap portion 4 with a pole gap portion 2 made of a non-magnetic material interposed therebetween. What is shown as 1a in the figure is the magnetic guide path for forming the main pole, and 1b in the figure is the magnetic guide path for forming the first adjacent pole,
The IC is a magnetic guide path for forming a second adjacent pole. Further, in the figure, reference numeral 5 denotes an overhang portion formed on the first adjacent pole forming magnetic guide path, and the overhang portion 5 is configured to protrude toward the main pole forming magnetic guide path 1a. The projecting portion may protrude toward the adjacent magnetic conduction path on the inner surface of the mold, that is, near the tip of the magnetic conduction path (for example, it may have a shape as shown in Fig. 3 or Fig. 4). Furthermore, as shown in FIG. 5, the projecting portion 5 can be directed toward the second adjacent pole forming magnetic guiding path 1c, which is the magnetic guiding path on the opposite side to the main pole forming magnetic guiding path 1a. A prominent configuration is also possible.
以下、本発明を具体的実施例に基づいて更に詳細に説明
するが、本発明はこれらにより制限されるものではない
。Hereinafter, the present invention will be explained in more detail based on specific examples, but the present invention is not limited thereto.
実施例
六方晶フェライト 90重量%(製品名
: GP330 、戸田工業■製)塩化ビニル樹脂
7.0重量%(製品名: 5100I
、鐘淵化学工業■製)DOP
2.8重量96トリベース 0
.1重量%ステアリン酸鉛 0.1重量
%上記配合物から作ったペレットを用いて直径14φ、
磁極数が3でラジアル磁界成分のピーク間角度として次
の値を持つマグネットロールを磁場配向押出成形した。Example Hexagonal ferrite 90% by weight (Product name: GP330, manufactured by Toda Kogyo ■) Vinyl chloride resin
7.0% by weight (Product name: 5100I
, manufactured by Kanebuchi Chemical Industry Co., Ltd.) DOP
2.8 weight 96 tribase 0
.. 1% by weight lead stearate 0.1% by weight Using pellets made from the above formulation, diameter 14φ,
A magnetic roll having three magnetic poles and the following value as the peak-to-peak angle of the radial magnetic field component was formed by magnetically oriented extrusion molding.
/5−N1=115℃
/Nl −N2= 120℃
/N2− S = 125℃
主極はS極であり、そのパタンのN1極側を急峻化する
とする。これを達成するため第1図に示すダイスを用い
各導磁路をヨーク毎に設けられた電磁石に磁気的に結合
させS極用励磁コイルに10000 AT (アンペア
・ターン)、N1、N2極用励磁コイルに3000A
T相当の直流電流を通しつつ押出成形した。又、比較例
として第2図に示すダイスにて同様の条件にて押出成形
した。第2図として示したダイスはS極形成用導磁路並
びにN2極形成用導磁路は第1図のものと同様てあり、
又、Nll影形成用導磁路マグネットロール外表面に相
対する部分の巾は第1図のものと同様であるが、ダイス
外径部にいたるまで幅広に形成し、張出部をなくした点
が第1図のものと相違している。/5-N1=115°C /Nl-N2=120°C/N2-S=125°C The main pole is the S pole, and the N1 pole side of the pattern is made steeper. To achieve this, we used the die shown in Figure 1 to magnetically couple each magnetic conduction path to an electromagnet provided for each yoke, and connected the excitation coil for the S pole to 10,000 AT (ampere turns) for the N1 and N2 poles. 3000A for excitation coil
Extrusion molding was carried out while passing a direct current equivalent to T. In addition, as a comparative example, extrusion molding was carried out using the die shown in FIG. 2 under the same conditions. The die shown in FIG. 2 has the same magnetic conductive path for forming the S pole and the magnetic guiding path for forming the N2 pole as in FIG.
In addition, the width of the part of the Nll shadow forming magnetic guide path facing the outer surface of the magnet roll is the same as that in Figure 1, but it is made wider up to the outer diameter of the die, and the overhanging part is eliminated. is different from that in Fig. 1.
得られた2つのマグネットロールのラジアル磁界成分(
N2)の絶対値の回転角に対する分布を第6図に示した
。実線で示したものが第1図で示したダイスを用いた場
合の分布てあり、破線で示したものが第2図で示したダ
イスを用いた場合の分布である。主極であるS極のパタ
ンの非対称度を便宜的に数値化するため次のパラメータ
を用いることにする。即ち、ピークからベースラインに
下ろした垂線とピーク値の半分の高さを示す水平線との
交点から該パタンの両端までの距離の比、即ち、第6図
において、!!、、!!、C1,≦12)の比/ !/
/Iを非対称度A、S、D (Asymmetryde
gree)と定義する。この非対称度を用いて2つのマ
グネットロールを評価したところ、ともにA。The radial magnetic field components of the two magnet rolls obtained (
The distribution of the absolute value of N2) with respect to the rotation angle is shown in FIG. The solid line shows the distribution when the die shown in FIG. 1 is used, and the broken line shows the distribution when the die shown in FIG. 2 is used. In order to conveniently quantify the degree of asymmetry of the pattern of the S pole, which is the main pole, the following parameters will be used. That is, the ratio of the distance from the intersection of the perpendicular line drawn from the peak to the baseline and the horizontal line indicating half the height of the peak value to both ends of the pattern, that is, in FIG. ! ,,! ! , C1,≦12)/! /
/I is the degree of asymmetry A, S, D (Asymmetric
gree). When two magnet rolls were evaluated using this degree of asymmetry, both received an A rating.
S、D=1.9であり十分非対称化されていることがわ
かった。しかし比較例にあってはNl極のパタンか広範
囲にわたり過ぎ、且つピーク値も低く、マグネットロー
ルとしての使用に耐えないものであることがわかった。It was found that S and D were 1.9, indicating that the asymmetric structure was sufficiently achieved. However, in the comparative example, the Nl electrode pattern was too wide and the peak value was too low, making it unsuitable for use as a magnet roll.
これに対して、本発明方法により作られたマグネットロ
ールにあってはN1極の磁界パタンはその分布範囲が絞
られており、ピーク値も高い値が実現できることが確認
された。On the other hand, it was confirmed that in the magnet roll made by the method of the present invention, the distribution range of the magnetic field pattern of the N1 pole is narrowed, and a high peak value can be achieved.
尚、前述した実施例では、外周部の形状は断面円形のも
ののみを対称としたが、本発明のマグネットロールは、
少なくとも主極から第1隣接極にいたる迄の領域がマグ
ネットロール外周における円弧の一部を構成していれば
他の形状であってもよく、例えば、主極から第1隣接極
にいたる領域以外の部分において、位置決め等の目的の
為に、外周面に平坦なカット面を設けたものも含まれる
。In addition, in the above-mentioned embodiment, the shape of the outer peripheral portion was symmetrical only with a circular cross section, but the magnet roll of the present invention has a symmetrical shape.
Other shapes may be used as long as at least the region from the main pole to the first adjacent pole constitutes a part of the circular arc on the outer periphery of the magnet roll, for example, other than the region from the main pole to the first adjacent pole. This also includes those with a flat cut surface on the outer circumferential surface for purposes such as positioning.
又、磁場配向成形手段としては押出成形のみならず射出
成形、圧縮成形等の手段も必要に応じて選択できる。Further, as the magnetic field orientation molding means, not only extrusion molding but also injection molding, compression molding, etc. can be selected as necessary.
本発明によれば、磁界分布においてピーク僅か4゜
らその強度が該ピーク値の172となる迄の範囲におい
て、主極の磁界分布をピーク値を挟んで非対称とするこ
とが可能で、良好なコピー画質を実現できるマグネット
ロールを得ることができる。そして、本発明によって得
られるマグネットロールは、単に主極の磁界分布が非対
称となるだけでなく、磁界分布を急峻化したい側に位置
する隣接極の磁界パタンか広範囲に広がったり、低レベ
ル化することもなく、マグネットロールとしての基本機
能を損なうこともない。しかも、このような優れた特性
を有するマグネットロールは、一体成形によって作成す
ることができるうえに、マグネットロール表面に凹部、
凸部、V字溝を形成する等の後加工の必要もないので、
量産性に優れるとともに、金型磨耗による特性変化のお
それもない。According to the present invention, it is possible to make the magnetic field distribution of the main pole asymmetrical with respect to the peak value in the range from a peak of only 4 degrees to a strength of 172 degrees of the peak value, and a good result is obtained. A magnetic roll that can achieve copy image quality can be obtained. In addition, the magnetic roll obtained by the present invention not only has an asymmetrical magnetic field distribution at the main pole, but also has a magnetic field pattern that spreads over a wide range or has a lower level at the adjacent pole located on the side where the magnetic field distribution is desired to be steeper. There is no problem, and the basic function as a magnetic roll is not impaired. Moreover, a magnet roll with such excellent properties can be made by integral molding, and it also has recesses and grooves on the surface of the magnet roll.
There is no need for post-processing such as forming protrusions or V-shaped grooves.
In addition to being excellent in mass production, there is no fear of changes in characteristics due to mold wear.
第1図は本発明方法に使用したダイスの1実施例を示す
断面図、第2図は従来のダイスの1例を示す断面図、第
3図〜第5図は本発明方法に使用したダイスの他の実施
例の断面図、第6図は第1図及び第2図に示したダイス
を用いて成形したマグネットロールのラジアル磁界(H
l)パタン、第7図は従来のマグネットロールの1例で
ある。
1:ダイスヨーク部、1a:主極形成用導磁路、lb:
第1隣接極形成用導磁路、
lC:第2隣接極形成用導磁路、
2;極間部、 3:コア、
4:空隙部、 5:張り出し部。
第
図
第
図
ツクーイ)
第
斥
父
図
第
図Fig. 1 is a sectional view showing an example of a die used in the method of the present invention, Fig. 2 is a sectional view showing an example of a conventional die, and Figs. 3 to 5 are sectional views showing an example of a die used in the method of the present invention. FIG. 6 is a sectional view of another embodiment of the radial magnetic field (H) of the magnet roll formed using the die shown in FIGS.
l) Pattern: Figure 7 is an example of a conventional magnetic roll. 1: Dice yoke part, 1a: Main pole forming magnetic guide path, lb:
1st adjacent pole forming magnetic guide path, 1C: 2nd adjacent pole forming magnetic guide path, 2; interpolar portion, 3: core, 4: gap portion, 5: overhang portion. (Fig. (Fig. Tsukui)) Fig. 1.
Claims (5)
主極の磁界のピーク値からその強度が少なくとも1/2
になる迄の範囲内の分布波形がピーク値を挟んで実質的
に非対称形であり、且つ該主極からそれに隣接する2つ
の磁極のうち少なくとも1つの磁極までを含む領域の外
周が実質的に円弧の一部である極異方配向により着磁さ
れた樹脂結合型の一体成形したマグネットロール。(1) In the circumferential pattern of the radial magnetic field component, the intensity is at least 1/2 from the peak value of the magnetic field of any main pole.
The distribution waveform within the range up to is substantially asymmetrical across the peak value, and the outer periphery of the region including from the main pole to at least one of the two adjacent magnetic poles is substantially A resin-bonded, integrally molded magnet roll that is magnetized by polar anisotropic orientation that is part of a circular arc.
主極の磁界のピーク値からその強度が1/3になる迄の
範囲内の分布波形がピーク値を挟んで実質的に非対称形
である請求項1記載のマグネットロール。(2) A claim that in the circumferential pattern of the radial magnetic field component, the distribution waveform within the range from the peak value of the magnetic field of any main pole until the intensity becomes 1/3 is substantially asymmetrical with the peak value in between. The magnetic roll according to item 1.
主極の磁界のピーク値からその強度が少なくとも1/2
になる迄の範囲内の分布波形がピーク値を挟んで実質的
に非対称形であり、且つ該主極からそれに隣接する2つ
の磁極のうち少なくとも1つの磁極までを含む領域の外
周が実質的に円弧の一部である極異方配向により着磁さ
れた樹脂結合型の一体成形したマグネットロールの成形
において、主極に隣接する2つの磁極のうち主極の磁界
パタンが急峻になる側に位置する磁極を形成する為の導
磁路の先端近傍に、隣接する磁極形成用の導磁路に向か
う突出部を形成した成形金型を用いたことを特徴とする
マグネットロールの製造方法。(3) In the circumferential pattern of the radial magnetic field component, the intensity is at least 1/2 from the peak value of the magnetic field of any main pole.
The distribution waveform within the range up to is substantially asymmetrical across the peak value, and the outer periphery of the region including from the main pole to at least one of the two adjacent magnetic poles is substantially In the molding of a resin-bonded integrally molded magnet roll that is magnetized by polar anisotropic orientation that is part of a circular arc, the magnetic field pattern of the main pole is located on the side where the magnetic field pattern of the main pole is steeper among the two magnetic poles adjacent to the main pole. A method for manufacturing a magnet roll, characterized in that a molding die is used in which a protrusion is formed near the tip of a magnetic guide path for forming a magnetic pole, and a protrusion toward an adjacent magnetic guide path for forming a magnetic pole.
磁路に向かわしめてなる請求項3記載のマグネットロー
ルの製造方法。(4) The method for manufacturing a magnet roll according to claim 3, wherein the protrusion formed near the tip of the magnetic guide path is directed toward the magnetic guide path for forming the main pole.
磁路の存在する側と反対側に存在する導磁路に向かわし
めてなる請求項3記載のマグネットロールの製造方法。(5) The method of manufacturing a magnet roll according to claim 3, wherein the protruding portion formed near the tip of the magnetic guide path is directed toward the magnetic guide path that exists on the opposite side to the side where the main pole forming magnetic guide path exists.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP26203090A JP2646823B2 (en) | 1990-09-29 | 1990-09-29 | Magnet roll and manufacturing method thereof |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP26203090A JP2646823B2 (en) | 1990-09-29 | 1990-09-29 | Magnet roll and manufacturing method thereof |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH04139706A true JPH04139706A (en) | 1992-05-13 |
JP2646823B2 JP2646823B2 (en) | 1997-08-27 |
Family
ID=17370055
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP26203090A Expired - Lifetime JP2646823B2 (en) | 1990-09-29 | 1990-09-29 | Magnet roll and manufacturing method thereof |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP2646823B2 (en) |
-
1990
- 1990-09-29 JP JP26203090A patent/JP2646823B2/en not_active Expired - Lifetime
Also Published As
Publication number | Publication date |
---|---|
JP2646823B2 (en) | 1997-08-27 |
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