JPS6354078B2 - - Google Patents
Info
- Publication number
- JPS6354078B2 JPS6354078B2 JP18525480A JP18525480A JPS6354078B2 JP S6354078 B2 JPS6354078 B2 JP S6354078B2 JP 18525480 A JP18525480 A JP 18525480A JP 18525480 A JP18525480 A JP 18525480A JP S6354078 B2 JPS6354078 B2 JP S6354078B2
- Authority
- JP
- Japan
- Prior art keywords
- sleeve
- plating
- magnet
- magnetic
- rotating
- 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
Links
- 239000000696 magnetic material Substances 0.000 claims description 4
- 238000005498 polishing Methods 0.000 claims description 4
- 238000007743 anodising Methods 0.000 claims description 2
- 238000009713 electroplating Methods 0.000 claims description 2
- 238000003672 processing method Methods 0.000 claims 2
- 238000004381 surface treatment Methods 0.000 claims 1
- 238000007747 plating Methods 0.000 description 33
- PXHVJJICTQNCMI-UHFFFAOYSA-N nickel Substances [Ni] PXHVJJICTQNCMI-UHFFFAOYSA-N 0.000 description 21
- 229910052759 nickel Inorganic materials 0.000 description 11
- 150000002500 ions Chemical class 0.000 description 10
- 238000000034 method Methods 0.000 description 10
- 238000010586 diagram Methods 0.000 description 5
- 230000000694 effects Effects 0.000 description 5
- 230000005684 electric field Effects 0.000 description 5
- 239000003792 electrolyte Substances 0.000 description 5
- 238000003754 machining Methods 0.000 description 4
- MUBZPKHOEPUJKR-UHFFFAOYSA-N Oxalic acid Chemical compound OC(=O)C(O)=O MUBZPKHOEPUJKR-UHFFFAOYSA-N 0.000 description 3
- 150000001768 cations Chemical class 0.000 description 3
- 230000004907 flux Effects 0.000 description 3
- 239000007788 liquid Substances 0.000 description 3
- 229910021645 metal ion Inorganic materials 0.000 description 3
- 239000000243 solution Substances 0.000 description 3
- VYZAMTAEIAYCRO-UHFFFAOYSA-N Chromium Chemical compound [Cr] VYZAMTAEIAYCRO-UHFFFAOYSA-N 0.000 description 2
- QAOWNCQODCNURD-UHFFFAOYSA-N Sulfuric acid Chemical compound OS(O)(=O)=O QAOWNCQODCNURD-UHFFFAOYSA-N 0.000 description 2
- 229910052782 aluminium Inorganic materials 0.000 description 2
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 2
- 150000002815 nickel Chemical class 0.000 description 2
- 230000003647 oxidation Effects 0.000 description 2
- 238000007254 oxidation reaction Methods 0.000 description 2
- 239000002245 particle Substances 0.000 description 2
- 230000003746 surface roughness Effects 0.000 description 2
- 230000009471 action Effects 0.000 description 1
- 235000019270 ammonium chloride Nutrition 0.000 description 1
- 239000007864 aqueous solution Substances 0.000 description 1
- 230000008859 change Effects 0.000 description 1
- KRVSOGSZCMJSLX-UHFFFAOYSA-L chromic acid Substances O[Cr](O)(=O)=O KRVSOGSZCMJSLX-UHFFFAOYSA-L 0.000 description 1
- 239000002131 composite material Substances 0.000 description 1
- 238000005260 corrosion Methods 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 238000005034 decoration Methods 0.000 description 1
- 239000008151 electrolyte solution Substances 0.000 description 1
- AWJWCTOOIBYHON-UHFFFAOYSA-N furo[3,4-b]pyrazine-5,7-dione Chemical compound C1=CN=C2C(=O)OC(=O)C2=N1 AWJWCTOOIBYHON-UHFFFAOYSA-N 0.000 description 1
- 230000005389 magnetism Effects 0.000 description 1
- 230000007246 mechanism Effects 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- LGQLOGILCSXPEA-UHFFFAOYSA-L nickel sulfate Chemical compound [Ni+2].[O-]S([O-])(=O)=O LGQLOGILCSXPEA-UHFFFAOYSA-L 0.000 description 1
- 229910000363 nickel(II) sulfate Inorganic materials 0.000 description 1
- 235000006408 oxalic acid Nutrition 0.000 description 1
- 230000002093 peripheral effect Effects 0.000 description 1
- 230000008569 process Effects 0.000 description 1
- 230000004044 response Effects 0.000 description 1
- 238000007788 roughening Methods 0.000 description 1
- 238000005488 sandblasting Methods 0.000 description 1
- 229910001220 stainless steel Inorganic materials 0.000 description 1
- 239000010935 stainless steel Substances 0.000 description 1
Landscapes
- Electrical Discharge Machining, Electrochemical Machining, And Combined Machining (AREA)
- Electrochemical Coating By Surface Reaction (AREA)
- Electroplating Methods And Accessories (AREA)
Description
本発明は内部にマグネツトを有する回転対称物
体表面を電解作用を利用して表面加工を行う方法
に関するものであり、例えば現像器のマグネツト
スリーブの表面に電解メツキ、陽極酸化、電解研
摩等の電解加工を施す方法である。
本発明においてマグネツトを内蔵する回転対称
物体とは電子写真用現像器のマグネツトスリーブ
の他に各種のマグネツトカツプリング、発電機等
がある。
具体的には例えば、自転車用発電機等の低コス
ト物の外面を防食装飾のためにメツキを施す場合
本発明により発電機を組立後にメツキを施すこと
ができメツキ後のキズを防ぐことができまた、均
一にメツキするため外観をそこねることもない。
次に本発明を電子写真用現像スリーブについて
詳述する。一般に電子写真用現像スリーブの耐久
性向上のため現像スリーブの表面硬質化方法とし
て、表面を電解メツキ、又は陽極酸化処理するこ
とが行なわれている。而して1成分現像方式に用
いる永久磁石ロールには、磁石回転形式、又はス
リーブ回転形式、あるいは、磁石とスリーブが相
対的に回転する複合式等がありそのロールの構造
は、非磁性材の円筒形スリーブの内周面に対し、
磁極が交互に異磁極を構成するように配置し、該
スリーブの軸方向にその全幅にわたつて磁石を設
ける磁石構成体あるいはこの磁石構成体の磁極の
一部に溝を設け、磁力分布波形に凹凸を生ぜしめ
るごとく構成する磁石構成体がシヤフトにより軸
支され、スリーブと相対して回転自在になるよう
設けられている。
このスリーブの表面に磁力によつて吸引された
現像剤は、スリーブに対し突設するドクタープレ
ートによつて所定の厚みに調整されて、スリーブ
または磁石構成体の回転によつて、磁気ブラシ極
の方に搬送され、スリーブ軸方向の現像有効幅全
域にわたつて均一なケバ立ち状態の現像剤により
現像用ローラに対しブラシを形成するものであ
る。
上述のごとく構成され作動する従来の永久磁石
ロールにおいては、スリーブとドクタープレート
とのギヤツプは0.1〜0.7mm程度と、高い外周精度
が要求される。すなわちその精度は、一般に真円
度が0.02〜0.03mm、円筒度が0.03〜0.05mm、磁石
構成体に対するスリーブの外周の振出しが0.05mm
以下という高精度である。
従つて、通常の引抜法で製作されるアルミ等の
導電性を有する非磁性材スリーブは、引抜きのま
までは上述のような高精度が要求される1成分現
像方式には使用できない。そこで一般に、このス
リーブ外周は、旋盤加工や無芯研摩盤加工等で1
〜30μmオーダーの表面粗度に加工されている。
而してこのような現像スリーブ表面を電解加工す
るに際し、次の2通りの方法が考えられる。
1) スリーブ表面のみを先に加工して後にマグ
ネツト軸フランジを取りつける。
2) 先にスリーブにマグネツト軸フランジなど
を取りつけたあとに、スリーブの表面加工を行
なう。
而して1)の場合電解加工上の問題点はスリー
ブへの電圧印加法、スリーブの保持方法、スリー
ブの外表面だけでなく内面にも不要な加工をする
こと、また電解加工以外の処理すなわち表面の研
摩、粗面化の作業がしにくいなどの欠点がある。
一方2)の場合内部にマグネツトを入れた状態
でメツキ等を行なうと、メツキ層厚が磁界に対応
して変化してしまい好ましくない。メツキ層厚が
磁界により変化するメカニズムは以下のとおりで
ある(第1図参照)。
一般にメツキとは金属イオン(陽イオン)を含
むメツキ液中に被メツキ表面を浸し被メツキ物が
電位的に負になるように、かつ被メツキ表面に均
一な電界が加わるよう配置して行なう。若し磁場
がないときはメツキ液中の金属イオン(陽イオ
ン)は第1図中〓で示された方向と速度で電気力
により吸引され均一なメツキを行なうことができ
る。しかし磁場が存在すると、メツキ液中の金属
イオン(陽イオン)にはローレンツ力すなわち
=q(〓+〓×〓)
なる力が加わる。
第1図でbのように磁極付近では磁場の方向と
イオンの運動方向が平行或いは反平行のため図示
の如くになる。しかるにa及びcの地点ではイオ
ンは電気力による力の外に磁力により紙面と垂直
に力を受けることになる、ローレンツの式に示さ
れたごとくこの力はイオンの運動方向と磁界が直
交したときに最大となりその方向はaでは紙面に
対し裏から表への方向、cでは紙面に対し表から
裏への方向である。以上のような力がイオンに働
きa,cでイオンは円筒の軸方向にも運動する結
果磁極に対応してメツキむらが発生する。
一方第2図のようにスリーブ端部においては磁
束が中央部と異なるためやはりメツキむらを生じ
る。これに更に端部においては電場が一定でない
ためによるメツキむらも加わり、メツキの均一な
仕上に非常に悪影響がある。
本発明は上述の如き欠点を除去するためマグネ
ツトスリーブ等の内部にマグネツトを有すものの
電解加工に際し、内部のマグネツトを被加工面に
対し回転させることにより、磁界によるメツキむ
らを除去することを目的とするものである。また
このとき該スリーブ周囲に磁性体を配置する方法
を併用しても良く、これは端部での加工むらの改
善となる。
本発明において、内部のマグネツトを被加工面
に対し回転せしめるに際しては、内部マグネツト
の周速をv=μE以上とすることが好ましい。μ
は電解液中のイオンのモビリテイでEは電界強度
を示す。電解液中のイオンはこのスピードで移動
するので内部マグネツトの周速がこれ以上あれば
良いことになる。
μの値は H+ 349.8cm2/secV
Ag+ 61.9
Cu2+ 53.6(25℃水溶液)
程度でH+を例にとると、10V/cm程度の電界下
で、35cm/sec以上の周速があれば良いことにな
り、直径30mmのスリーブでは180rpmとなる。
被電解加工物を回転させる理由は次の通りであ
る。
一般にCr2+ Ni2+ Cu+等のイオンは磁性を示す
ため前述のローレンツ力以外にも各イオンの磁気
双極子に磁界による力が働き、磁極に対応したメ
ツキむらは更にひどくなる。このような磁性イオ
ンに対してもスリーブを回転させることは有効で
ある。
実施例 1
電子写真用の現像スリーブとして、第1図に示
した4極マグネツトロールを内蔵したステンレス
(SUS304)スリーブを用いた。スリーブ表面の
磁束密度は各々700Gである。上記スリーブ表面
を粒度 #600の不定形粒子でサンドブラストした
後に硬質化するために少量の硫酸を含むクロム酸
メツキ液(液組成CrO3300g/、SO2- 4/CrO3=
1/100)中でメツキ液温度40℃、電流密度18A/
dm2で5μ厚の硬質クロムメツキを施したところス
リーブ内の磁極に対応してメツキむらを生じた。
これは外見上はつきりと識別できその厚みむらは
数十%におよぶものであつた。
これに対し本発明により第3図に示すごとくス
リーブ2は固定しスリーブ内のマグネツト1を外
部から回転手段5により100〜500rpmで回転させ
たところ厚みむらのない均一なハードクロムメツ
キが得られた。図中3は電解液、4はスリーブ支
持体、6は電解槽、7は電源を示す。本例ではス
リーブの両端部をメツキせずにマスクすることが
必要であつたため端部の一方はスリーブの固定部
材4により、他方はシールによりマスキングして
おく。このような場合にはメツキ層両端のメツキ
むらは問題とならなかつた。
実施例 2
第4図に示す実施態様で両端部にも均一にメツ
キするため磁性体(ニツケル)のメツシユ8をス
リーブ2の周囲に配し、実施例1と同様にマグネ
ツト1を回転させながらかつニツケルメツシユ8
を陽極としてニツケルメツキを施した。スリーブ
2としては実施例1と同様のものを用いた。この
ようにするとスリーブ端部の磁束は第5図のよう
になり第2図の場合と比し均一磁場を得ることが
できた。またニツケルメツシユの電極効果により
電界も均一となるため、端部においても均一なメ
ツキ厚を得ることができた。このニツケルメツシ
ユは、50〜200メツシユのものを使用した。この
ニツケルとしては、電解ニツケル、ロールニツケ
ル、デポラライズドニツケル、カーボナイズドニ
ツケル等の純度の高いものが良い。また電解液は
NiSO4―NH4Cl―H3BO3で、20℃〜35℃、0.5〜
1A/dm2の条件下でメツキを行なう。このニツ
ケルメツシユはスリーブ径の1.5〜3.0倍の直径の
円筒状に加工し、スリーブと同メツシユは同軸上
におかれる。
実施例 3
20℃の2%シユウ酸電解液中でアルミニウム製
スリーブを陽極として、電圧100V、電流密度2.0
A/dm2で陽極酸化を施し表面にアルマイトを形
成時、実施例1と同様にマグネツトを100〜
500rpmで回転させて実施したところ均一なアル
マイト層が得られた。
実施例 4
第6図に示すようにメツキ槽6を回転磁界中に
おきスリーブ2内のマグネツトを回転せしめつ
つ、他は実施例1と同様に実施した。回転磁界と
して、8極のものを使用し50Hzの交流電流をコイ
ル9に流したところスリーブ内マグネツト1は約
600rpmで回転し実施例1と同様の効果が得られ
た。図中10は継鉄を示す。
次に各実施例における表面粗さを表1に示す。
The present invention relates to a method of surface processing a rotationally symmetrical object surface having a magnet inside by using electrolytic action. This is a method of processing. In the present invention, rotationally symmetrical objects containing magnets include various magnetic couplings, generators, etc. in addition to the magnetic sleeve of an electrophotographic developing device. Specifically, for example, when plating the outer surface of a low-cost product such as a bicycle generator for anti-corrosion decoration, the present invention allows the plating to be applied after the generator is assembled, thereby preventing scratches after plating. Also, since it is plated uniformly, the appearance will not be damaged. Next, the present invention will be explained in detail regarding a developing sleeve for electrophotography. Generally, in order to improve the durability of electrophotographic developing sleeves, the surface of the developing sleeve is subjected to electrolytic plating or anodic oxidation treatment as a method of hardening the surface. The permanent magnet rolls used in the one-component development system include a magnet rotation type, a sleeve rotation type, or a composite type in which a magnet and a sleeve rotate relative to each other. For the inner circumferential surface of the cylindrical sleeve,
A magnet structure in which magnetic poles are arranged so as to alternately constitute different magnetic poles, and magnets are provided over the entire width in the axial direction of the sleeve, or a groove is provided in a part of the magnetic poles of this magnet structure, and the magnetic force distribution waveform is A magnet structure configured to produce unevenness is supported by a shaft and is provided so as to be freely rotatable relative to the sleeve. The developer magnetically attracted to the surface of the sleeve is adjusted to a predetermined thickness by a doctor plate that protrudes from the sleeve, and is applied to the magnetic brush pole by rotation of the sleeve or magnet structure. A brush is formed on the developing roller by the developer in a uniform fluffy state over the entire effective width of development in the axial direction of the sleeve. In the conventional permanent magnet roll constructed and operated as described above, the gap between the sleeve and the doctor plate is approximately 0.1 to 0.7 mm, and high circumferential precision is required. In other words, the accuracy is generally 0.02 to 0.03 mm for roundness, 0.03 to 0.05 mm for cylindricity, and 0.05 mm for the outer circumference of the sleeve relative to the magnet structure.
The accuracy is as follows. Therefore, a conductive non-magnetic material sleeve made of aluminum or the like manufactured by a normal drawing method cannot be used in the one-component development method that requires high accuracy as described above if it is drawn as is. Therefore, in general, the outer circumference of this sleeve is processed by lathe processing or coreless polishing machine processing, etc.
Processed to a surface roughness of ~30μm order.
When electrolytically processing the surface of such a developing sleeve, the following two methods can be considered. 1) Process only the sleeve surface first and then attach the magnetic shaft flange. 2) After attaching the magnetic shaft flange etc. to the sleeve, perform surface processing on the sleeve. In the case of 1), the problems with electrolytic machining include the method of applying voltage to the sleeve, the method of holding the sleeve, unnecessary machining not only on the outer surface of the sleeve but also on the inner surface, and processing other than electrolytic machining. It has drawbacks such as difficulty in polishing and roughening the surface. On the other hand, in case 2), if plating is performed with a magnet inside, the thickness of the plating layer will change in response to the magnetic field, which is undesirable. The mechanism by which the plating layer thickness changes depending on the magnetic field is as follows (see Figure 1). Generally, plating is carried out by immersing the surface to be plated in a plating solution containing metal ions (cations) and arranging the object to be plated so that the potential is negative and a uniform electric field is applied to the surface to be plated. If there is no magnetic field, the metal ions (cations) in the plating solution are attracted by the electric force in the direction and speed shown by ⓓ in FIG. 1, and uniform plating can be performed. However, when a magnetic field exists, the Lorentz force, ie, the force =q(〓+〓×〓) is applied to the metal ions (cations) in the plating liquid. In the vicinity of the magnetic pole, as shown in b in FIG. 1, the direction of the magnetic field and the direction of ion movement are parallel or antiparallel, resulting in the state shown in the figure. However, at points a and c, in addition to the electric force, the ion is subjected to a force perpendicular to the plane of the paper due to the magnetic force. The direction is the direction from the back to the front with respect to the paper surface in a, and the direction from the front to the back with respect to the paper surface in c. The above forces act on the ions and the ions move in the axial direction of the cylinder at points a and c, resulting in uneven plating in correspondence with the magnetic poles. On the other hand, as shown in FIG. 2, the magnetic flux at the ends of the sleeve is different from that at the center, which also causes uneven plating. In addition to this, there is also the uneven plating caused by the uneven electric field at the edges, which has a very negative effect on the uniform finish of the plating. In order to eliminate the above-mentioned drawbacks, the present invention is designed to remove uneven plating caused by the magnetic field by rotating the internal magnet relative to the surface to be machined during electrolytic machining of items that have a magnet inside, such as a magnetic sleeve. This is the purpose. Further, at this time, a method of arranging a magnetic material around the sleeve may also be used, which improves processing unevenness at the end. In the present invention, when rotating the internal magnet with respect to the surface to be machined, it is preferable that the circumferential speed of the internal magnet be set to v=μE or more. μ
is the mobility of ions in the electrolyte and E is the electric field strength. Since ions in the electrolyte move at this speed, it is sufficient if the peripheral speed of the internal magnet is higher than this. The value of μ is approximately H + 349.8cm 2 /secV Ag + 61.9 Cu 2+ 53.6 (25℃ aqueous solution). Taking H + as an example, under an electric field of approximately 10V/cm, a circumferential speed of 35cm/sec or more is obtained. This would be a good thing, and for a sleeve with a diameter of 30mm, it would be 180rpm. The reason for rotating the electrolytically processed object is as follows. In general, ions such as Cr 2+ Ni 2+ Cu + exhibit magnetism, so in addition to the Lorentz force described above, a force due to the magnetic field acts on the magnetic dipole of each ion, making the plating unevenness corresponding to the magnetic pole even worse. Rotating the sleeve is also effective against such magnetic ions. Example 1 A stainless steel (SUS304) sleeve with a built-in four-pole magnet roll shown in FIG. 1 was used as a developing sleeve for electrophotography. The magnetic flux density on each sleeve surface is 700G. After sandblasting the sleeve surface with irregularly shaped particles of particle size #600, a chromic acid plating solution containing a small amount of sulfuric acid (liquid composition CrO 3 300g/, SO 2- 4 /CrO 3 =
1/100), plating liquid temperature 40℃, current density 18A/
When hard chrome plating with a thickness of 5 μm was applied at dm 2 , uneven plating occurred corresponding to the magnetic poles inside the sleeve.
This was clearly visible from the outside, and the unevenness in thickness was several tens of percent. On the other hand, according to the present invention, as shown in Fig. 3, the sleeve 2 was fixed and the magnet 1 inside the sleeve was rotated from the outside at 100 to 500 rpm by the rotating means 5, and a uniform hard chrome plating with no uneven thickness was obtained. . In the figure, 3 is an electrolytic solution, 4 is a sleeve support, 6 is an electrolytic cell, and 7 is a power source. In this example, since it was necessary to mask both ends of the sleeve without plating, one end was masked with the fixing member 4 of the sleeve and the other with a seal. In such cases, uneven plating at both ends of the plating layer did not pose a problem. Example 2 In the embodiment shown in FIG. 4, a mesh 8 made of magnetic material (nickel) is arranged around the sleeve 2 in order to uniformly plate both ends. Nickel mesh 8
was used as an anode and nickel-metallic was applied. As the sleeve 2, the same one as in Example 1 was used. By doing this, the magnetic flux at the end of the sleeve became as shown in FIG. 5, and a more uniform magnetic field could be obtained than in the case of FIG. 2. Furthermore, because the electric field was made uniform due to the electrode effect of the nickel mesh, it was possible to obtain a uniform plating thickness even at the edges. This nickel mesh used was one with 50 to 200 mesh. As the nickel, those having high purity such as electrolytic nickel, rolled nickel, depolarized nickel, and carbonized nickel are preferable. Also, the electrolyte
NiSO4 - NH4Cl - H3BO3 , 20℃~35℃, 0.5~
Plating is performed under the condition of 1A/ dm2 . This nickel mesh is machined into a cylindrical shape with a diameter 1.5 to 3.0 times the diameter of the sleeve, and the sleeve and the mesh are placed coaxially. Example 3 In a 2% oxalic acid electrolyte at 20°C, using an aluminum sleeve as an anode, voltage 100V, current density 2.0
When anodic oxidation is performed at A/ dm2 to form alumite on the surface, the magnet is
When the test was carried out by rotating at 500 rpm, a uniform alumite layer was obtained. Example 4 The plating tank 6 was placed in a rotating magnetic field as shown in FIG. 6, and the magnet inside the sleeve 2 was rotated, but the other aspects were the same as in Example 1. When an 8-pole rotating magnetic field was used and a 50Hz alternating current was passed through the coil 9, the magnet 1 inside the sleeve was approximately
The same effect as in Example 1 was obtained by rotating at 600 rpm. In the figure, 10 indicates a yoke. Next, Table 1 shows the surface roughness in each example.
【表】
本発明は以上の実施例にも示す如く次の如く顕
著な効果を示すものである。マグネツトを回転さ
せる効果として
1 前述のように磁界の影響によるメツキムラを
防げる。
2 均一にメツキするためスリーブを回転せしめ
ると良いが、このときスリーブのまわりに泡が
発生しメツキを妨げる難点がある。本発明にお
いてはスリーブを固定しマグネツトを回転させ
ることによりイオン流を撹拌するため、均一な
メツキができる。
3 メツキあるいは陽極酸化、電解研摩等のスピ
ードとマグネツトの回転速度の選定により容易
に表面の仕上状態をコントロールできる。[Table] As shown in the above examples, the present invention exhibits the following remarkable effects. Effects of rotating the magnet: 1. As mentioned above, it prevents unevenness due to the influence of the magnetic field. 2. It is best to rotate the sleeve to ensure uniform plating, but this has the disadvantage that bubbles are generated around the sleeve and interfere with plating. In the present invention, the ion flow is stirred by fixing the sleeve and rotating the magnet, so uniform plating can be achieved. 3. The surface finish can be easily controlled by selecting the speed of plating, anodizing, electrolytic polishing, etc. and the rotation speed of the magnet.
第1図はメツキ層が磁界により変化する態様の
説明図、第2図はスリーブ端部における磁界変化
の態様の説明図、第3図、第4図は本発明の実施
例における実施態様の説明図、第5図は同実施例
における磁界変化を示す説明図、第6図は他の実
施例の実施態様の説明図である。
1:マグネツト軸、2:スリーブ、3:電解
液、4:スリーブ支持体、5:マグネツト回転部
材、6:電解槽、7:電源、8:ニツケルメツシ
ユ、9:コイル、10:継鉄。
Fig. 1 is an explanatory diagram of the manner in which the plating layer changes due to the magnetic field, Fig. 2 is an explanatory diagram of the manner in which the magnetic field changes at the end of the sleeve, and Figs. 3 and 4 are explanatory diagrams of the embodiment of the embodiment of the present invention. FIG. 5 is an explanatory diagram showing changes in the magnetic field in the same embodiment, and FIG. 6 is an explanatory diagram of an embodiment of another embodiment. 1: Magnetic shaft, 2: Sleeve, 3: Electrolyte, 4: Sleeve support, 5: Magnetic rotating member, 6: Electrolytic cell, 7: Power source, 8: Nickel mesh, 9: Coil, 10: Yoke.
Claims (1)
面を電解メツキ、陽極酸化電解研摩等の電解加工
するに際し、該現像用スリーブを固定し該マグネ
ツトを回転させることを特徴とする表面加工法。 2 現像用スリーブの周囲に磁性体を配置するこ
とを特徴とする特許請求の範囲第1項記載の表面
加工法。 3 現像用スリーブを回転磁性中に配置すること
を特徴とする特許請求の範囲第1項記載の表面加
工法。[Scope of Claims] 1. A surface treatment characterized by fixing the developing sleeve and rotating the magnet when performing electrolytic processing such as electrolytic plating or anodizing electrolytic polishing on the surface of a developing sleeve having a magnet inside. Law. 2. The surface processing method according to claim 1, characterized in that a magnetic material is arranged around the developing sleeve. 3. The surface processing method according to claim 1, characterized in that the developing sleeve is placed in a rotating magnet.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP18525480A JPS57110689A (en) | 1980-12-26 | 1980-12-26 | Surface working method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP18525480A JPS57110689A (en) | 1980-12-26 | 1980-12-26 | Surface working method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS57110689A JPS57110689A (en) | 1982-07-09 |
| JPS6354078B2 true JPS6354078B2 (en) | 1988-10-26 |
Family
ID=16167590
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP18525480A Granted JPS57110689A (en) | 1980-12-26 | 1980-12-26 | Surface working method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS57110689A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP3219831B1 (en) | 2014-11-14 | 2019-03-27 | YKK Corporation | Surface electrolytic treatment method for clothing accessory components, clothing accessories, and production method therefor |
| US10626515B2 (en) | 2014-11-14 | 2020-04-21 | Ykk Corporation | Surface electrolytic treatment apparatus for garment accessory part |
-
1980
- 1980-12-26 JP JP18525480A patent/JPS57110689A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS57110689A (en) | 1982-07-09 |
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