JP2011248311A - Ferrite particle for electrostatically charging magnetic brush and manufacturing method of the same - Google Patents

Ferrite particle for electrostatically charging magnetic brush and manufacturing method of the same Download PDF

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JP2011248311A
JP2011248311A JP2010124447A JP2010124447A JP2011248311A JP 2011248311 A JP2011248311 A JP 2011248311A JP 2010124447 A JP2010124447 A JP 2010124447A JP 2010124447 A JP2010124447 A JP 2010124447A JP 2011248311 A JP2011248311 A JP 2011248311A
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ferrite particles
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magnetic brush
ferrite
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JP5567396B2 (en
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Yoshiaki Aiki
良明 相木
Toshiya Kitamura
利哉 北村
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Dowa Electronics Materials Co Ltd
Dowa IP Creation Co Ltd
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Abstract

PROBLEM TO BE SOLVED: To provide ferrite particles for electrostatically charging a magnetic brush in which electric resistance is not fluctuated or reduced even when it is used for a long period of time and stable electrostatic chargeability is obtained.SOLUTION: The ferrite particle contains as a principal component a material represented by the general formula: MnFeO(wherein 0≤x≤1), and has a surface roughness of 0.4 to 0.6 μm and a saturation magnetization of 60 emu/g or more. A difference between before crushing and after crushing of a peak intensity ratio of FeOto MnFeOobtained from X-ray diffraction is set 0.015 or less in the absolute value. Al is preferably 0.2 to 2.0 mass% in aluminum and dissolved. An electric resistance value at an applied voltage of 1000 V is preferably within the range from 1.0×10Ω to 9.0×10Ω.

Description

本発明は磁気ブラシ帯電用のフェライト粒子及びその製造方法に関するものである。   The present invention relates to ferrite particles for charging a magnetic brush and a method for producing the same.

電子写真方式の画像形成装置では、これまでコロトロンやスコロトロンといった感光体と接触しないコロナ帯電装置が広く用いられてきた。ところが、近年の環境意識の高まりを受けて、オゾンが不可避的に発生するコロナ帯電装置に代わって、オゾンを発生しない接触型の帯電装置が注目され、種々の装置が開発実用化されつつある。   In electrophotographic image forming apparatuses, corona charging devices such as corotrons and scorotrons that do not come into contact with photoreceptors have been widely used. However, in response to the recent increase in environmental awareness, contact-type charging devices that do not generate ozone have attracted attention in place of corona charging devices that inevitably generate ozone, and various devices are being developed and put into practical use.

接触型の帯電装置としては、ローラ帯電装置や固定ブラシ帯電装置、磁気ブラシ帯電装置などがあり、これらの中でも長寿命や感光体上の残留トナーの回収等の点から磁気ブラシ帯電装置が注目されている。磁気ブラシ帯電装置は、磁性粒子を磁気力で担持体表面にブラシ状に担持し、この磁気ブラシを感光体に接触させるとともに電圧を印加し感光体を帯電させるものである(例えば、特許文献1を参照)。   As the contact type charging device, there are a roller charging device, a fixed brush charging device, a magnetic brush charging device, etc. Among them, the magnetic brush charging device attracts attention from the viewpoints of long life and recovery of residual toner on the photoreceptor. ing. The magnetic brush charging device carries magnetic particles in the form of a brush on the surface of a carrier by magnetic force, and contacts the magnetic brush with a photoconductor and applies a voltage to charge the photoconductor (for example, Patent Document 1). See).

磁気ブラシを構成する磁性粒子としては、磁気ブラシから離脱しない所定の磁気力と、感光体を帯電させる所定の電気抵抗とを有する必要がある。このため、使用する磁性粒子としては、例えば焼成したフェライト粒子を酸化処理したり、コート樹脂で表面被覆したりして電気抵抗の調整を行っていた。   The magnetic particles constituting the magnetic brush must have a predetermined magnetic force that does not separate from the magnetic brush and a predetermined electric resistance that charges the photosensitive member. For this reason, as the magnetic particles to be used, for example, the fired ferrite particles are oxidized or the surface is coated with a coating resin to adjust the electric resistance.

特開平8-254881号公報JP-A-8-254881

しかしながら、酸化処理や表面被覆したフェライト粒子を長期間にわたって使用すると、粒子表面の摩耗や欠け等によって電気抵抗が変動・低下する不具合が生じる。   However, when the oxidation-treated or surface-coated ferrite particles are used for a long period of time, there is a problem that the electric resistance fluctuates or decreases due to wear or chipping on the particle surface.

本発明はこのような従来の問題に鑑みてなされたものであり、その目的は、長期間使用しても電気抵抗が変動・低下することなく、また帯電ムラが抑制された磁気ブラシ帯電用のフェライト粒子を提供することにある。   The present invention has been made in view of such a conventional problem, and the object of the present invention is to provide a magnetic brush for charging, in which electrical resistance does not fluctuate or decrease even when used for a long period of time, and charging unevenness is suppressed. It is to provide ferrite particles.

また本発明の目的は、前記特性を有する磁気ブラシ帯電用のフェライト粒子を効率的に製造する方法を提供することにある。   Another object of the present invention is to provide a method for efficiently producing ferrite particles for charging a magnetic brush having the above characteristics.

本発明によれば、一般式MnFe3−x(但し、0≦x≦1)で表される材料を主成分とし、磁気ブラシ帯電に用いられるフェライト粒子であって、粒子の表面粗さが0.4〜0.6μmの範囲で、飽和磁化が60emu/g以上であり、X線回折で得られるFeとMnFeとのピーク強度比の、粉砕前と粉砕後の差が絶対値で0.015以下であることを特徴とするフェライト粒子が提供される。 According to the present invention, ferrite particles comprising a material represented by the general formula Mn x Fe 3-x O 4 (where 0 ≦ x ≦ 1) as a main component and used for magnetic brush charging, Before and after pulverization of the peak intensity ratio of Fe 2 O 3 and MnFe 2 O 4 obtained by X-ray diffraction with a roughness in the range of 0.4 to 0.6 μm and a saturation magnetization of 60 emu / g or more. Ferrite particles characterized in that the subsequent difference is 0.015 or less in absolute value are provided.

なお、本明細書における粒子の表面粗さRaは、JIS B 0601で規定される算術平均粗さをいうものとする。また、X線回折(「XRD」:X‐ray diffraction)の測定条件は後述の実施例で示す。   In addition, the surface roughness Ra of the particle in this specification shall mean the arithmetic average roughness prescribed | regulated by JIS B 0601. The measurement conditions of X-ray diffraction (“XRD”: X-ray diffraction) are shown in the examples described later.

ここで、粒子の表面粗さを前記範囲とする観点からは、Alを、Al換算で0.2〜2.0重量%固溶させるのが好ましい。   Here, from the viewpoint of setting the surface roughness of the particles in the above range, it is preferable to dissolve Al in an amount of 0.2 to 2.0% by weight in terms of Al.

また、感光体等の被帯電体を効果的に帯電させる観点からは、印加電圧1000Vのときのフェライト粒子の電気抵抗値を1×10〜1×10Ωの範囲とするのが好ましい。 In addition, from the viewpoint of effectively charging a member to be charged such as a photoreceptor, it is preferable that the electric resistance value of the ferrite particles when the applied voltage is 1000 V is in the range of 1 × 10 6 to 1 × 10 8 Ω.

そしてまた、本発明によれば、一般式MnFe3−x(但し、0≦x≦1)で表わされる組成のフェライト粒子が生成するように成分調整されたFe原料とMn原料、及びAl原料を媒体液中で混合してスラリーを得る工程と、前記スラリーを噴霧乾燥させて造粒物を得る工程と、酸素濃度が1.0〜1.7%の範囲で前記造粒物を焼成して焼成物を得る工程とを有することを特徴とする磁気ブラシ帯電用のフェライト粒子の製造方法が提供される。 According to the present invention, the Fe raw material and the Mn raw material whose components are adjusted so that ferrite particles having a composition represented by the general formula Mn x Fe 3-x O 4 (where 0 ≦ x ≦ 1) are generated, And a step of mixing an Al raw material in a medium solution to obtain a slurry, a step of spray-drying the slurry to obtain a granulated product, and the granulated product in an oxygen concentration range of 1.0 to 1.7%. There is provided a method for producing ferrite particles for charging a magnetic brush, characterized in that the method comprises a step of obtaining a fired product by firing.

Al原料の添加量としては、Al換算で0.2〜2.0重量%の範囲が好ましい。   The addition amount of the Al raw material is preferably in the range of 0.2 to 2.0% by weight in terms of Al.

本発明に係る磁気ブラシ帯電用のフェライト粒子によれば、長期間使用しても電気抵抗が変動・低下することなく、また帯電ムラが抑制される。   According to the ferrite particles for charging a magnetic brush according to the present invention, the electrical resistance does not fluctuate or decrease even when used for a long period of time, and charging unevenness is suppressed.

また本発明に係るフェライト粒子の製造方法によれば、磁気ブラシ帯電用のフェライト粒子を効率的に製造することができる。   Further, according to the method for producing ferrite particles according to the present invention, ferrite particles for charging a magnetic brush can be efficiently produced.

磁気ブラシ帯電装置の一例を示す概説図である。It is a schematic diagram which shows an example of a magnetic brush charging device. 実施例3のフェライト粒子のSEM写真である。4 is a SEM photograph of ferrite particles of Example 3. 実施例1における感光体ドラムの表面電位の経時変化を示す図である。FIG. 3 is a diagram illustrating a change with time of the surface potential of the photosensitive drum in Embodiment 1. 実施例1のフェライト粒子のXRD測定結果を示すグラフである。4 is a graph showing the XRD measurement results of the ferrite particles of Example 1. 比較例4のフェライト粒子のSEM写真である。4 is a SEM photograph of ferrite particles of Comparative Example 4. 比較例4における感光体ドラムの表面電位の経時変化を示す図である。FIG. 10 is a diagram showing a change with time in the surface potential of the photosensitive drum in Comparative Example 4;

まず、磁気ブラシ帯電装置について簡単に説明する。図1に、磁気ブラシ帯電装置の一例を示す概説図を示す。この図に示す磁気ブラシ帯電装置1は、アルミニウム等の非磁性材料からなる回転自在の磁気スリーブ11と、磁気スリーブ11内に固定配置された、周方向に異なる磁極が着磁されたマグネットロール12と、マグネットロール12の磁気力で磁気スリーブ11の外周に磁気ブラシを形成する磁性粒子13とを備える。そして、磁気ブラシ帯電装置1は、被帯電体としての感光体ドラム2の表面に磁気ブラシが接触しニップ部が形成されるように配設されている。また、磁気スリーブ11には電圧印加電源3が接続されている。磁気スリーブ11及び感光体ドラム2は時計回りに回転する。すなわち、ニップ部において磁気スリーブ11は感光体ドラム2の回転方向に対してカウンター方向に回転する。   First, the magnetic brush charging device will be briefly described. FIG. 1 is a schematic diagram showing an example of a magnetic brush charging device. A magnetic brush charging device 1 shown in this figure includes a rotatable magnetic sleeve 11 made of a nonmagnetic material such as aluminum, and a magnet roll 12 fixedly arranged in the magnetic sleeve 11 and magnetized with different magnetic poles in the circumferential direction. And magnetic particles 13 that form a magnetic brush on the outer periphery of the magnetic sleeve 11 by the magnetic force of the magnet roll 12. The magnetic brush charging device 1 is arranged so that the magnetic brush contacts the surface of the photosensitive drum 2 as a member to be charged and a nip portion is formed. A voltage application power source 3 is connected to the magnetic sleeve 11. The magnetic sleeve 11 and the photosensitive drum 2 rotate clockwise. That is, the magnetic sleeve 11 rotates in the counter direction with respect to the rotation direction of the photosensitive drum 2 in the nip portion.

このような構成の磁気ブラシ帯電装置1において、感光体ドラム2を帯電させる場合には、磁気スリーブ11を回転させると共に磁気スリーブ11に電圧印加電源3から所定電圧を印加する。すると、磁気スリーブ11の回転と共に磁気ブラシも同方向に回転し、ニップ部において磁気ブラシが感光体ドラム2の表面を摺擦し感光体ドラム2が接触帯電される。   In the magnetic brush charging device 1 having such a configuration, when charging the photosensitive drum 2, the magnetic sleeve 11 is rotated and a predetermined voltage is applied to the magnetic sleeve 11 from the voltage application power source 3. Then, the magnetic brush rotates in the same direction as the magnetic sleeve 11 rotates, and the magnetic brush rubs the surface of the photosensitive drum 2 at the nip portion, and the photosensitive drum 2 is contact-charged.

なお、磁気スリーブ11を設けることなく、マグネットロール12を回転自在とし、その表面に磁気ブラシを形成するように磁気ブラシ帯電装置を構成しても構わない。   Note that the magnetic brush charging device may be configured such that the magnet roll 12 is rotatable and the magnetic brush is formed on the surface thereof without providing the magnetic sleeve 11.

以上のような磁気ブラシ帯電装置1の磁性粒子として本発明に係るフェライト粒子は好適に使用される。本発明に係るフェライト粒子の大きな特徴の一つは、組成式:MnFe3−x(但し、0≦x≦1)で表される材料を主成分とし、粒子の表面粗さを0.4〜0.6μmの範囲としたことにある。フェライト粒子の表面粗さを前記範囲とすることによって、感光体などの被帯電体をムラなく帯電させることができるようになる。粒子の表面粗さが0.4μm未満であると、被帯電体の帯電ムラが大きくなる一方、0.6μmを超えると、磁気ブラシの穂が硬くなり、表面の凸部が被帯電体に強く摺擦されことにより、表面を傷つける可能性がある。 The ferrite particles according to the present invention are preferably used as the magnetic particles of the magnetic brush charging device 1 as described above. One of the major characteristics of the ferrite particles according to the present invention is that the main component is a material represented by the composition formula: Mn x Fe 3-x O 4 (where 0 ≦ x ≦ 1), and the surface roughness of the particles is It is in the range of 0.4 to 0.6 μm. By setting the surface roughness of the ferrite particles in the above range, it becomes possible to charge a charged body such as a photosensitive member without unevenness. When the surface roughness of the particles is less than 0.4 μm, the charged unevenness of the object to be charged becomes large. On the other hand, when it exceeds 0.6 μm, the ears of the magnetic brush become hard, and the convex portions on the surface are strong against the object to be charged. The surface may be damaged by rubbing.

フェライト粒子の表面粗さを前記範囲とするには、例えば、後述するフェライト粒子の製造工程においてAl成分を添加すればよい。Al成分を添加することによって、MnFe3−x結晶構造中のMnがAlに置き換わり、結晶成長速度の違いが生じて粒子表面に凹凸ができる。フェライト粒子の表面粗さを前記範囲とするには、Al成分の固溶量はAl換算で0.2〜2.0重量%の範囲とするのが好ましい。 In order to make the surface roughness of the ferrite particles within the above range, for example, an Al component may be added in the ferrite particle manufacturing process described later. By adding Al component, replace the Mn x Fe 3-x O 4 Mn in the crystal structure is Al, it is uneven particle surface resulting crystal growth rate difference. In order to make the surface roughness of the ferrite particles in the above range, the solid solution amount of the Al component is preferably in the range of 0.2 to 2.0% by weight in terms of Al.

また、本発明に係るフェライト粒子は飽和磁化σが60emu/g以上であることが重要である。飽和磁化σが60emu/g未満であると、フェライト粒子の被帯電体への付着が頻繁に起きるおそれがある。一方、飽和磁化の好適な上限値は80emu/gである。飽和磁化σが80emu/gを超えると、磁気ブラシの穂が硬くなり被帯電体を傷つけるおそれがある。フェライト粒子の、より好ましい飽和磁化σは60〜80emu/gの範囲である。 Further, it is important that the ferrite particles according to the present invention have a saturation magnetization σ s of 60 emu / g or more. If the saturation magnetization σ s is less than 60 emu / g, the ferrite particles may frequently adhere to the member to be charged. On the other hand, a suitable upper limit of saturation magnetization is 80 emu / g. When the saturation magnetization σ s exceeds 80 emu / g, the ears of the magnetic brush become hard and there is a risk of damaging the charged body. The more preferable saturation magnetization σ s of the ferrite particles is in the range of 60 to 80 emu / g.

本発明に係るフェライト粒子の好ましい電気抵抗は、印加電圧1000Vにおいて1.0×10〜9.0×10Ωcmの範囲である。フェライト粒子の電気抵抗が1.0×10よりも低いと、電荷のリークが起きるおそれがある一方、電気抵抗が9.0×10Ωcmを超えると、非帯電体に電荷を均一に注入できないおそれがある。フェライト粒子の、より好ましい電気抵抗は4.0×10〜9.0×10Ωcmの範囲である。なお、具体的測定条件は後述の実施例において記述する。 The preferred electrical resistance of the ferrite particles according to the present invention is in the range of 1.0 × 10 6 to 9.0 × 10 8 Ωcm at an applied voltage of 1000V. If the electrical resistance of the ferrite particles is lower than 1.0 × 10 6 , charge leakage may occur, while if the electrical resistance exceeds 9.0 × 10 8 Ωcm, the charge is uniformly injected into the uncharged body. It may not be possible. A more preferable electric resistance of the ferrite particles is in the range of 4.0 × 10 6 to 9.0 × 10 7 Ωcm. Specific measurement conditions will be described in the examples described later.

また、磁気ブラシ帯電装置に使用されるフェライト粒子の電気抵抗は、長時間の使用による経時変化が小さいことが重要である。電気抵抗の経時変化は、FeとMnFeの比率の差が、表面と内部で小さいと低減される。本発明に係るフェライト粒子は、当該粒子のX線回折で得られるFeとMnFeとのピーク強度比の、粉砕前と粉砕後の差が絶対値で0.015以下であることが重要である。粉砕前と粉砕後の差が絶対値で0.015より高いと、FeとMnFeの組成比率が表面と内部で大きく異なり、粒子表面に摩耗や欠けが生じた時、電気抵抗が変動・低下する不具合を発生させるおそれがある。 In addition, it is important that the electrical resistance of the ferrite particles used in the magnetic brush charging device is small in change over time due to long-term use. The change in electrical resistance with time is reduced when the difference in the ratio of Fe 2 O 3 and MnFe 2 O 4 is small between the surface and the inside. In the ferrite particles according to the present invention, the absolute value of the difference between the peak intensity ratio of Fe 2 O 3 and MnFe 2 O 4 obtained by X-ray diffraction of the particles before and after pulverization is 0.015 or less. This is very important. When the difference between before and after pulverization is higher than 0.015 in absolute value, the composition ratio of Fe 2 O 3 and MnFe 2 O 4 is greatly different between the surface and the inside, and when the particle surface is worn or chipped, There is a risk that the resistance may fluctuate or decrease.

本発明に係るフェライト粒子の平均粒子径としては10μm〜100μmの範囲が好ましい。平均粒子径が10μm以上あることで、粒子のそれぞれに必要な磁力が確実に付与され、例えば、感光体などの被帯電体へのフェライト粒子の付着が抑制されるようになる。一方、平均粒子径が100μm以下であることで、帯電ムラが一層抑制されるようになる。フェライト粒子の平均粒子径を上記範囲とするには、フェライト粒子の製造工程中または製造工程後に篩等を用いて分級処理を行えばよい。   The average particle diameter of the ferrite particles according to the present invention is preferably in the range of 10 μm to 100 μm. When the average particle diameter is 10 μm or more, a necessary magnetic force is reliably applied to each of the particles, and for example, adhesion of ferrite particles to a charged body such as a photoreceptor is suppressed. On the other hand, when the average particle size is 100 μm or less, uneven charging is further suppressed. In order to set the average particle diameter of the ferrite particles within the above range, classification may be performed using a sieve or the like during the manufacturing process of the ferrite particles or after the manufacturing process.

本発明のフェライト粒子の製造方法に特に限定はないが、以下に説明する製造方法が好適である。   Although the manufacturing method of the ferrite particle of the present invention is not particularly limited, the manufacturing method described below is preferable.

まず、Fe原料とMn原料、Al原料とを秤量して分散媒中に投入し混合してスラリーを作製する。Fe原料としては、Fe粉、Fe酸化物、Fe水酸化物等が使用でき、Mn原料としては、MnFe仮焼粉、Mn酸化物、Mn水酸化物等が好適に使用できる。Al原料としてはAlが好適に使用できる。 First, a Fe raw material, a Mn raw material, and an Al raw material are weighed, put into a dispersion medium, and mixed to prepare a slurry. As the Fe raw material, Fe 2 O 3 powder, Fe oxide, Fe hydroxide, etc. can be used. As the Mn raw material, MnFe 2 O 4 calcined powder, Mn oxide, Mn hydroxide, etc. are suitably used. it can. Al 2 O 3 can be suitably used as the Al raw material.

ここで重要なことはAl原料を添加することにある。Al原料を添加することによって、MnFe3−x結晶構造中のMnがAlに置き換わり、グレインの成長性に大きさ差が生じて粒子表面に凹凸ができる。フェライト粒子の表面粗さを0.4〜0.6μmの範囲とするには、Al原料の添加量をAl換算で0.2〜2.0重量%の範囲とするのが好ましい。 What is important here is to add an Al raw material. By adding the Al raw material, Mn in the Mn x Fe 3-x O 4 crystal structure is replaced with Al, and the grain growth is caused to have a difference in size, and the particle surface is uneven. In order to make the surface roughness of the ferrite particles in the range of 0.4 to 0.6 μm, it is preferable that the addition amount of the Al raw material is in the range of 0.2 to 2.0% by weight in terms of Al.

Al原料の添加量は前記のように微量であることから、Fe原料及びMn原料よりも先にAl原料を分散媒に投入し分散させてもよい。原スラリーの固形分濃度は50〜90wt%の範囲が望ましい。原料であるFe原料、Mn原料、Al原料を分散媒に投入する前に、必要により、粉砕混合処理しておいてもよい。   Since the addition amount of the Al raw material is very small as described above, the Al raw material may be introduced into the dispersion medium and dispersed before the Fe raw material and the Mn raw material. The solid content concentration of the raw slurry is desirably in the range of 50 to 90 wt%. If necessary, the raw material Fe raw material, Mn raw material, and Al raw material may be pulverized and mixed before being introduced into the dispersion medium.

本発明で使用する分散媒としては水が好適である。分散媒には、前記Fe原料、Mn原料、Al原料の他、必要によりバインダー、分散剤等を配合してもよい。バインダーとしては、例えば、ポリビニルアルコールが好適に使用できる。バインダーの配合量としてはスラリー中の濃度が0.5〜2wt%程度とするのが好ましい。また、分散剤としては、例えば、ポリカルボン酸アンモニウム等が好適に使用できる。分散剤の配合量としてはスラリー中の濃度が0.5〜2wt%程度とするのが好ましい。その他、潤滑剤や焼結促進剤等を配合してもよい。   Water is preferred as the dispersion medium used in the present invention. In addition to the Fe raw material, Mn raw material, and Al raw material, a binder, a dispersing agent, and the like may be blended in the dispersion medium as necessary. For example, polyvinyl alcohol can be suitably used as the binder. The blending amount of the binder is preferably about 0.5 to 2 wt% in the slurry. Moreover, as a dispersing agent, polycarboxylate ammonium etc. can be used conveniently, for example. As the blending amount of the dispersant, the concentration in the slurry is preferably about 0.5 to 2 wt%. In addition, you may mix | blend a lubricant, a sintering accelerator, etc.

次に、以上のようにして作製されたスラリーを必要により湿式粉砕する。例えば、ボールミルや振動ミルを用いて所定時間湿式粉砕する。粉砕後の原材料の平均粒径は50μm以下が好ましく、より好ましくは10μm以下である。振動ミルやボールミルには、所定粒径のメディアを内在させるのがよい。メディアの材質としては、鉄系のクロム鋼や酸化物系のジルコニア、チタニア、アルミナなどが挙げられる。粉砕工程の形態としては連続式及び回分式のいずれであってもよい。粉砕物の粒径は、粉砕時間や回転速度、使用するメディアの材質・粒径などによって調整される。   Next, the slurry prepared as described above is wet-pulverized as necessary. For example, wet grinding is performed for a predetermined time using a ball mill or a vibration mill. The average particle diameter of the raw material after pulverization is preferably 50 μm or less, more preferably 10 μm or less. The vibration mill or ball mill preferably contains a medium having a predetermined particle diameter. Examples of the material of the media include iron-based chromium steel and oxide-based zirconia, titania, and alumina. As a form of a grinding | pulverization process, any of a continuous type and a batch type may be sufficient. The particle size of the pulverized product is adjusted depending on the pulverization time and rotation speed, the material and particle size of the media used, and the like.

そして、粉砕されたスラリーを噴霧乾燥させて造粒する。具体的には、スプレードライヤーなどの噴霧乾燥機にスラリーを導入し、雰囲気中へ噴霧することによって球状に造粒する。噴霧乾燥時の雰囲気温度は100〜300℃の範囲が好ましい。これにより、粒径10〜200μmの球状の造粒物が得られる。なお、得られた造粒物は、振動ふるい等を用いて、粗大粒子や微粉を除去し粒度分布をシャープなものとするのが望ましい。   Then, the pulverized slurry is spray-dried and granulated. Specifically, the slurry is introduced into a spray dryer such as a spray dryer, and granulated into a spherical shape by spraying into the atmosphere. The atmospheric temperature during spray drying is preferably in the range of 100 to 300 ° C. Thereby, a spherical granulated product having a particle size of 10 to 200 μm is obtained. In addition, it is desirable that the obtained granulated product has a sharp particle size distribution by removing coarse particles and fine powder using a vibration sieve or the like.

次に、得られた造粒物を加熱した炉に投入して焼成し、磁性相を有する焼成物を得る。焼成温度は、目的となる磁性相が生成する温度範囲に設定すればよいが、本発明に係るフェライト粒子を製造する場合には、1000〜1400℃の温度範囲で焼成することが好ましい。より好ましくは、1100℃〜1350℃の温度範囲である。   Next, the obtained granulated product is put into a heated furnace and fired to obtain a fired product having a magnetic phase. The firing temperature may be set to a temperature range in which the target magnetic phase is generated. However, when producing the ferrite particles according to the present invention, firing is preferably performed in a temperature range of 1000 to 1400 ° C. More preferably, it is the temperature range of 1100 degreeC-1350 degreeC.

ここで重要なことは、焼結工程における酸素濃度を1.0〜1.7%の範囲とすることである。従来は窒素雰囲気下(酸素濃度200〜300ppm程度)で焼結を行い、粒子内部まで均一にフェライト化させて飽和磁化等の磁気特性を向上させていた。一方、粒子内部まで均一にフェライト化させると電気抵抗が低下するため、従来は製造の最終工程においてフェライト粒子を酸化処理して所定の電気抵抗を得ていた。ところが、酸化処理したフェライト粒子を使用すると、経時劣化により粒子表面に摩耗や欠けが生じ電気抵抗が低下する不具合が生じる。そこで本発明では、焼成工程における酸素濃度を従来よりも高くして粒子内部に均一にヘマタイト層を形成し、電気抵抗の経時安定性を図った。   What is important here is that the oxygen concentration in the sintering step is in the range of 1.0 to 1.7%. Conventionally, sintering was performed under a nitrogen atmosphere (oxygen concentration of about 200 to 300 ppm), and the inside of the particles was uniformly ferritized to improve magnetic characteristics such as saturation magnetization. On the other hand, when ferrite is uniformly formed into the inside of the particle, the electric resistance is lowered. Conventionally, the ferrite particles are oxidized in the final manufacturing process to obtain a predetermined electric resistance. However, when oxidized ferrite particles are used, the surface of the particles is worn or chipped due to deterioration over time, resulting in a problem that the electric resistance is lowered. Therefore, in the present invention, the oxygen concentration in the firing process is made higher than before, and a hematite layer is uniformly formed inside the particles, so that the stability of electrical resistance with time is achieved.

焼結工程における酸素濃度が1.0%未満であると、粒子内部に均一にヘマタイト層が形成されない一方、酸素濃度が1.7%を超えると、飽和磁化などの磁気特性が低下する。より好ましい酸素濃度としては1.2〜1.6%の範囲である。   If the oxygen concentration in the sintering process is less than 1.0%, a hematite layer is not uniformly formed inside the particles. On the other hand, if the oxygen concentration exceeds 1.7%, magnetic properties such as saturation magnetization are deteriorated. A more preferable oxygen concentration is in the range of 1.2 to 1.6%.

次に、得られた焼成物を解砕する。具体的には、例えば、ハンマーミル等によって焼成物を解砕する。解砕工程の形態としては連続式及び回分式のいずれであってもよい。そして、必要により、粒径を所定範囲に揃えるため分級を行ってもよい。分級方法としては、風力分級や篩分級など従来公知の方法を用いることができる。また、風力分級機で1次分級した後、振動篩や超音波篩で粒径を所定範囲に揃えるようにしてもよい。さらに、分級工程後に、磁場選鉱機によって非磁性粒子を除去するようにしてもよい。   Next, the obtained fired product is crushed. Specifically, for example, the fired product is crushed by a hammer mill or the like. As a form of a crushing process, any of a continuous type and a batch type may be sufficient. And if necessary, classification may be performed in order to make the particle size in a predetermined range. As a classification method, a conventionally known method such as air classification or sieve classification can be used. In addition, after primary classification with an air classifier, the particle size may be aligned within a predetermined range with a vibration sieve or an ultrasonic sieve. Furthermore, you may make it remove a nonmagnetic particle with a magnetic field separator after a classification process.

以上のようにして作製した本発明のフェライト粒子は帯電用磁気ブラシとしてそのまま使用される。また、必要により粒子表面を樹脂で被覆して使用してもよい。   The ferrite particles of the present invention produced as described above are used as they are as a charging magnetic brush. If necessary, the particle surface may be coated with a resin.

フェライト粒子の表面を被覆する樹脂としては、従来公知のものが使用でき、例えば、ポリエチレン、ポリプロピレン、ポリ塩化ビニル、ポリ−4−メチルペンテン−1、ポリ塩化ビニリデン、ABS(アクリロニトリル−ブタジエン−スチレン)樹脂、ポリスチレン、(メタ)アクリル系樹脂、ポリビニルアルコール系樹脂、並びにポリ塩化ビニル系やポリウレタン系、ポリエステル系、ポリアミド系、ポリブタジエン系等の熱可塑性エストラマー、フッ素シリコーン系樹脂などが挙げられる。   As the resin for covering the surface of the ferrite particles, conventionally known resins can be used, for example, polyethylene, polypropylene, polyvinyl chloride, poly-4-methylpentene-1, polyvinylidene chloride, ABS (acrylonitrile-butadiene-styrene). Examples thereof include resins, polystyrene, (meth) acrylic resins, polyvinyl alcohol resins, polyvinyl chloride-based, polyurethane-based, polyester-based, polyamide-based, polybutadiene-based thermoplastic elastomers, fluorine silicone-based resins, and the like.

フェライト粒子の表面を樹脂で被覆するには、樹脂の溶液又は分散液をフェライト粒子に施せばよい。塗布溶液用の溶媒としては、トルエン、キシレン等の芳香族炭化水素系溶媒;アセトン、メチルエチルケトン、メチルイソブチルケトン、シクロヘキサノン等のケトン系溶媒;テトラヒドロフラン、ジオキサン等の環状エーテル類溶媒;エタノール、プロパノール、ブタノール等のアルコール系溶媒;エチルセロソルブ、ブチルセロソルブ等のセロソルブ系溶媒;酢酸エチル、酢酸ブチル等のエステル系溶媒;ジメチルホルムアミド、ジメチルアセトアミド等のアミド系溶媒などの1種又は2種以上を用いることができる。塗布溶液中の樹脂成分濃度は、一般に0.001〜30wt%、特に0.001〜2wt%の範囲内にあるのがよい。   In order to coat the surface of the ferrite particles with a resin, a resin solution or dispersion may be applied to the ferrite particles. Solvents for the coating solution include aromatic hydrocarbon solvents such as toluene and xylene; ketone solvents such as acetone, methyl ethyl ketone, methyl isobutyl ketone, and cyclohexanone; cyclic ether solvents such as tetrahydrofuran and dioxane; ethanol, propanol, and butanol Alcohol solvents such as ethyl cellosolve, cellosolve solvents such as butyl cellosolve; ester solvents such as ethyl acetate and butyl acetate; amide solvents such as dimethylformamide and dimethylacetamide, etc. . The concentration of the resin component in the coating solution is generally in the range of 0.001 to 30 wt%, particularly 0.001 to 2 wt%.

フェライト粒子への樹脂の被覆方法としては、例えばスプレードライ法や流動床法あるいは流動床を用いたスプレードライ法、浸漬法等を用いることができる。これらの中でも、少ない樹脂量で効率的に塗布できる点で流動床法が特に好ましい。樹脂被覆量は、例えば流動床法の場合には吹き付ける樹脂溶液量や吹き付け時間によって調整することができる。   As a method for coating the resin on the ferrite particles, for example, a spray drying method, a fluidized bed method, a spray drying method using a fluidized bed, an immersion method, or the like can be used. Among these, the fluidized bed method is particularly preferable in that it can be efficiently applied with a small amount of resin. For example, in the case of the fluidized bed method, the resin coating amount can be adjusted by the amount of resin solution sprayed and the spraying time.

(実施例1)
平均粒径が約1μmに微粉砕されたAl粉と、Feと、Mnとを準備した。そして、Al粉をAl換算で5000ppm、Feと、Mnを8:2(モル比)となるように秤量した。分散剤としてポリカルボン酸アンモニウムを、媒体液中濃度が1%となるように添加した純水中に、秤量したAlとFe、Mnとを分散させ混合物とした。この混合物を湿式ボールミル(メディア径2mm)で粉砕処理し、スラリーを得た。
Example 1
Al 2 O 3 powder finely pulverized to an average particle diameter of about 1 μm, Fe 2 O 3 and Mn 3 O 4 were prepared. Then, 5000 ppm of Al 2 O 3 powder in terms of Al, and Fe 2 O 3, the Mn 3 O 4 8: two were weighed such that the molar ratio. Weighed Al 2 O 3 , Fe 2 O 3 , and Mn 3 O 4 were dispersed in pure water to which ammonium polycarboxylate as a dispersant was added so that the concentration in the medium liquid was 1% to obtain a mixture. . This mixture was pulverized by a wet ball mill (media diameter: 2 mm) to obtain a slurry.

得られたスラリーをスプレードライヤーにて約150℃の熱風中に噴霧し、粒径10〜100μmの乾燥造粒物を得た。そして、篩を用いて粒径が100μmを超える造粒物を除去した。得られた乾燥造粒物を、電気炉に投入して、酸素濃度1.6%の窒素雰囲気下にて、1100℃で3時間焼成して焼成物を得た。得られた焼成物を粉砕処理した後、篩を用いて粗粒及び微粒を除去し、平均粒子径45μmのMnフェライト粒子を得た。なお、フェライト粒子の平均粒子径は、レーザー回折式粒度分布測定装置(日機装株式会社製マイクロトラック、Model 9320−X100)を用いて測定したものである。   The obtained slurry was sprayed into hot air at about 150 ° C. with a spray dryer to obtain a dry granulated product having a particle size of 10 to 100 μm. And the granulated material with a particle size exceeding 100 micrometers was removed using the sieve. The obtained dried granulated product was put into an electric furnace and fired at 1100 ° C. for 3 hours in a nitrogen atmosphere having an oxygen concentration of 1.6% to obtain a fired product. After the obtained fired product was pulverized, coarse particles and fine particles were removed using a sieve to obtain Mn ferrite particles having an average particle diameter of 45 μm. The average particle size of the ferrite particles is measured using a laser diffraction particle size distribution measuring device (Microtrack, Model 9320-X100 manufactured by Nikkiso Co., Ltd.).

得られたフェライト粒子の表面粗さ、飽和磁化σs、帯電性、X線回折を下記方法で測定した。結果を表1に示す。また、感光体ドラムの表面電位の経時変化を図3に、XRD測定結果を図4にそれぞれ示す。   The surface roughness, saturation magnetization σs, chargeability, and X-ray diffraction of the obtained ferrite particles were measured by the following methods. The results are shown in Table 1. FIG. 3 shows the time-dependent change in the surface potential of the photosensitive drum, and FIG. 4 shows the XRD measurement results.

(表面粗さ)
表面粗さRaは、レーザー顕微鏡(オリンパス社製LEXT OLS3000)により測定した。より詳細には、フェライト粒子において10μm四方の範囲を設定し、当該範囲において高さ測定を行って平均線を求め、この範囲での平均線から測定曲線までの偏差の絶対値を合成し、平均化することで算出した。
(Surface roughness)
The surface roughness Ra was measured with a laser microscope (OLYMPUS LEXT OLS3000). More specifically, a range of 10 μm square is set in the ferrite particles, the height is measured in the range to obtain an average line, and the absolute value of the deviation from the average line to the measurement curve in this range is synthesized, and the average It was calculated by converting.

(飽和磁化測定)
フェライトの磁気特性は、VSM(東英工業株式会社製、VSM−P7)を用いて磁化率の測定を行い、印加磁場10kOeにおける飽和磁化σ(emu/g)を測定した。
(Saturation magnetization measurement)
The magnetic properties of the ferrite were measured for magnetic susceptibility using VSM (manufactured by Toei Kogyo Co., Ltd., VSM-P7), and the saturation magnetization σ s (emu / g) in an applied magnetic field of 10 kOe was measured.

(帯電性)
図1に示した磁気ブラシ帯電装置を用いて感光体ドラムを帯電させ、その表面電位を非接触電圧測定装置(トレック社製)を用いて測定し、感光体ドラムの表面電位の経時変化を調べた。
(Chargeability)
The photosensitive drum is charged using the magnetic brush charging device shown in FIG. 1, the surface potential is measured using a non-contact voltage measuring device (manufactured by Trek), and the change in the surface potential of the photosensitive drum with time is examined. It was.

(電気抵抗測定)
表面を電解研磨した厚さ2mmの電極としての真鍮板2枚を、距離2mm離して対向するように配置した。電極間にフェライト粒子200mgを装入した後、それぞれの電極の背後に、断面積240mmの磁石(表面磁束密度が1500ガウスのフェライト磁石)を配置して、電極間にフェライト粒子のブリッジを形成させた。そして、10Vから1000Vまでの直流電圧を電極間に印加し、フェライト粒子に流れる電流値を測定し、フェライト粒子の電気抵抗を算出した。
(Electrical resistance measurement)
Two brass plates as electrodes having a thickness of 2 mm whose surfaces were electropolished were arranged to face each other with a distance of 2 mm. After inserting 200 mg of ferrite particles between the electrodes, a magnet having a cross-sectional area of 240 mm 2 (ferrite magnet having a surface magnetic flux density of 1500 gauss) is placed behind each electrode to form a bridge of ferrite particles between the electrodes. I let you. A DC voltage of 10 V to 1000 V was applied between the electrodes, the value of the current flowing through the ferrite particles was measured, and the electrical resistance of the ferrite particles was calculated.

(X線回折測定)
X線回折装置(リガク製、RINT2000)を用いて測定した。X線源はコバルトを使用し、加速電圧40kV、電流30mAでX線を発生させた。粉末X線の測定条件は走査モード:FT、発散スリット:1/2°、散乱スピード:1/2°、受光スリット:0.15mm、回転速度:5.000rpm、測定角度:10°≦2θ≦90°、測定間隔:0.01°、計数時間:5秒で測定を行った。
(X-ray diffraction measurement)
It measured using the X-ray-diffraction apparatus (Rigaku make, RINT2000). Cobalt was used as the X-ray source, and X-rays were generated at an acceleration voltage of 40 kV and a current of 30 mA. The measurement conditions of the powder X-ray are scanning mode: FT, divergence slit: 1/2 °, scattering speed: 1/2 °, light receiving slit: 0.15 mm, rotation speed: 5.000 rpm, measurement angle: 10 ° ≦ 2θ ≦ Measurement was performed at 90 °, measurement interval: 0.01 °, and counting time: 5 seconds.

(実施例2)
焼成温度を1150℃とした以外は、実施例1と同様にして焼成物を得た。得られた焼成物を粉砕処理した後、篩を用いて粗粒及び微粒を除去し、平均粒子径45μmのMnフェライト粒子を得た。
得られたフェライト粒子の表面粗さ、飽和磁化σs、帯電性、X線回折を実施例1と同様にして測定した。結果を表1に示す。
(Example 2)
A fired product was obtained in the same manner as in Example 1 except that the firing temperature was 1150 ° C. After the obtained fired product was pulverized, coarse particles and fine particles were removed using a sieve to obtain Mn ferrite particles having an average particle diameter of 45 μm.
The surface roughness, saturation magnetization σs, chargeability, and X-ray diffraction of the obtained ferrite particles were measured in the same manner as in Example 1. The results are shown in Table 1.

(実施例3)
焼成温度を1200℃とした以外は、実施例1と同様にして焼成物を得た。得られた焼成物を粉砕処理した後、篩を用いて粗粒及び微粒を除去し、平均粒子径45μmのMnフェライト粒子を得た。得られたフェライト粒子の電子顕微鏡(SEM)写真を図2に示す。
得られたフェライト粒子の表面粗さ、飽和磁化σs、帯電性、X線回折を実施例1と同様にして測定した。結果を表1に示す。
(Example 3)
A fired product was obtained in the same manner as in Example 1 except that the firing temperature was 1200 ° C. After the obtained fired product was pulverized, coarse particles and fine particles were removed using a sieve to obtain Mn ferrite particles having an average particle diameter of 45 μm. An electron microscope (SEM) photograph of the obtained ferrite particles is shown in FIG.
The surface roughness, saturation magnetization σs, chargeability, and X-ray diffraction of the obtained ferrite particles were measured in the same manner as in Example 1. The results are shown in Table 1.

(実施例4)
焼成工程における酸素濃度を1.0%とし、焼成温度を1200℃とした以外は、実施例1と同様にして焼成物を得た。得られた焼成物を粉砕処理した後、篩を用いて粗粒及び微粒を除去し、平均粒子径45μmのMnフェライト粒子を得た。
得られたフェライト粒子の表面粗さ、飽和磁化σs、帯電性、X線回折を実施例1と同様にして測定した。結果を表1に示す。
Example 4
A fired product was obtained in the same manner as in Example 1 except that the oxygen concentration in the firing step was 1.0% and the firing temperature was 1200 ° C. After the obtained fired product was pulverized, coarse particles and fine particles were removed using a sieve to obtain Mn ferrite particles having an average particle diameter of 45 μm.
The surface roughness, saturation magnetization σs, chargeability, and X-ray diffraction of the obtained ferrite particles were measured in the same manner as in Example 1. The results are shown in Table 1.

(実施例5)
焼成工程における酸素濃度を1.2%とし、焼成温度を1200℃とした以外は、実施例1と同様にして焼成物を得た。得られた焼成物を粉砕処理した後、篩を用いて粗粒及び微粒を除去し、平均粒子径45μmのMnフェライト粒子を得た。
得られたフェライト粒子の表面粗さ、飽和磁化σs、帯電性、X線回折を実施例1と同様にして測定した。結果を表1に示す。
(Example 5)
A fired product was obtained in the same manner as in Example 1 except that the oxygen concentration in the firing step was 1.2% and the firing temperature was 1200 ° C. After the obtained fired product was pulverized, coarse particles and fine particles were removed using a sieve to obtain Mn ferrite particles having an average particle diameter of 45 μm.
The surface roughness, saturation magnetization σs, chargeability, and X-ray diffraction of the obtained ferrite particles were measured in the same manner as in Example 1. The results are shown in Table 1.

(実施例6)
焼成工程における酸素濃度を1.4%とし、焼成温度を1200℃とした以外は、実施例1と同様にして焼成物を得た。得られた焼成物を粉砕処理した後、篩を用いて粗粒及び微粒を除去し、平均粒子径45μmのMnフェライト粒子を得た。
得られたフェライト粒子の表面粗さ、飽和磁化σs、帯電性、X線回折を実施例1と同様にして測定した。結果を表1に示す。
(Example 6)
A fired product was obtained in the same manner as in Example 1 except that the oxygen concentration in the firing step was 1.4% and the firing temperature was 1200 ° C. After the obtained fired product was pulverized, coarse particles and fine particles were removed using a sieve to obtain Mn ferrite particles having an average particle diameter of 45 μm.
The surface roughness, saturation magnetization σs, chargeability, and X-ray diffraction of the obtained ferrite particles were measured in the same manner as in Example 1. The results are shown in Table 1.

(比較例1)
焼成工程における酸素濃度を2.0%とし、焼成温度を1200℃とした以外は、実施例1と同様にして焼成物を得た。得られた焼成物を粉砕処理した後、篩を用いて粗粒及び微粒を除去し、平均粒子径45μmのMnフェライト粒子を得た。
得られたフェライト粒子の表面粗さ、飽和磁化σs、帯電性、X線回折を実施例1と同様にして測定した。結果を表1に示す。
(Comparative Example 1)
A fired product was obtained in the same manner as in Example 1 except that the oxygen concentration in the firing step was 2.0% and the firing temperature was 1200 ° C. After the obtained fired product was pulverized, coarse particles and fine particles were removed using a sieve to obtain Mn ferrite particles having an average particle diameter of 45 μm.
The surface roughness, saturation magnetization σs, chargeability, and X-ray diffraction of the obtained ferrite particles were measured in the same manner as in Example 1. The results are shown in Table 1.

(比較例2)
焼成工程における酸素濃度を2.5%とし、焼成温度を1200℃とした以外は、実施例1と同様にして焼成物を得た。得られた焼成物を粉砕処理した後、篩を用いて粗粒及び微粒を除去し、平均粒子径45μmのMnフェライト粒子を得た。
得られたフェライト粒子の表面粗さ、飽和磁化σs、帯電性、X線回折を実施例1と同様にして測定した。結果を表1に示す。
(Comparative Example 2)
A fired product was obtained in the same manner as in Example 1 except that the oxygen concentration in the firing step was 2.5% and the firing temperature was 1200 ° C. After the obtained fired product was pulverized, coarse particles and fine particles were removed using a sieve to obtain Mn ferrite particles having an average particle diameter of 45 μm.
The surface roughness, saturation magnetization σs, chargeability, and X-ray diffraction of the obtained ferrite particles were measured in the same manner as in Example 1. The results are shown in Table 1.

(比較例3)
Al粉を添加せず、焼成工程における焼成温度を1200℃とした以外は、実施例1と同様にして焼成物を得た。得られた焼成物を粉砕処理した後、篩を用いて粗粒及び微粒を除去し、平均粒子径45μmのMnフェライト粒子を得た。
得られたフェライト粒子の表面粗さ、飽和磁化σs、帯電性、X線回折を実施例1と同様にして測定した。結果を表1に示す。
(Comparative Example 3)
A fired product was obtained in the same manner as in Example 1 except that Al 2 O 3 powder was not added and the firing temperature in the firing step was 1200 ° C. After the obtained fired product was pulverized, coarse particles and fine particles were removed using a sieve to obtain Mn ferrite particles having an average particle diameter of 45 μm.
The surface roughness, saturation magnetization σs, chargeability, and X-ray diffraction of the obtained ferrite particles were measured in the same manner as in Example 1. The results are shown in Table 1.

(比較例4)
Al粉を添加せず、焼成工程における酸素濃度を0.03%とし、焼成温度を1200℃とした以外は、実施例1と同様にして焼成物を得た。得られた焼成物を粉砕処理した後、篩を用いて粗粒及び微粒を除去し、平均粒子径45μmのMnフェライト粒子を得た。得られたフェライト粒子を酸化処理(大気雰囲気下、450℃×1.5時間)した。
得られたフェライト粒子の表面粗さ、飽和磁化σs、帯電性、X線回折を実施例1と同様にして測定した。結果を表1に示す。また、得られたフェライト粒子の電子顕微鏡写真を図5に、感光体ドラムの表面電位の経時変化を図6にそれぞれ示す。
(Comparative Example 4)
A fired product was obtained in the same manner as in Example 1 except that Al 2 O 3 powder was not added, the oxygen concentration in the firing step was 0.03%, and the firing temperature was 1200 ° C. After the obtained fired product was pulverized, coarse particles and fine particles were removed using a sieve to obtain Mn ferrite particles having an average particle diameter of 45 μm. The obtained ferrite particles were oxidized (450 ° C. × 1.5 hours in an air atmosphere).
The surface roughness, saturation magnetization σs, chargeability, and X-ray diffraction of the obtained ferrite particles were measured in the same manner as in Example 1. The results are shown in Table 1. Further, FIG. 5 shows an electron micrograph of the obtained ferrite particles, and FIG. 6 shows changes with time in the surface potential of the photosensitive drum.

(比較例5)
焼成工程における酸素濃度を0.03%とし、焼成温度を1200℃とした以外は、実施例1と同様にして焼成物を得た。得られた焼成物を粉砕処理した後、篩を用いて粗粒及び微粒を除去し、平均粒子径45μmのMnフェライト粒子を得た。得られたフェライト粒子を酸化処理(大気雰囲気下、450℃×1.5時間)した。
得られたフェライト粒子の表面粗さ、飽和磁化σs、帯電性、X線回折を実施例1と同様にして測定した。結果を表1に示す。
(Comparative Example 5)
A fired product was obtained in the same manner as in Example 1 except that the oxygen concentration in the firing step was 0.03% and the firing temperature was 1200 ° C. After the obtained fired product was pulverized, coarse particles and fine particles were removed using a sieve to obtain Mn ferrite particles having an average particle diameter of 45 μm. The obtained ferrite particles were oxidized (450 ° C. × 1.5 hours in an air atmosphere).
The surface roughness, saturation magnetization σs, chargeability, and X-ray diffraction of the obtained ferrite particles were measured in the same manner as in Example 1. The results are shown in Table 1.

(比較例6)
Al粉を添加せず、焼成工程における酸素濃度を0.03%とした以外は、実施例1と同様にして焼成物を得た。得られた焼成物を粉砕処理した後、篩を用いて粗粒及び微粒を除去し、平均粒子径45μmのMnフェライト粒子を得た。
得られたフェライト粒子の表面粗さ、飽和磁化σs、帯電性、X線回折を実施例1と同様にして測定した。結果を表1に示す。
(Comparative Example 6)
A fired product was obtained in the same manner as in Example 1 except that Al 2 O 3 powder was not added and the oxygen concentration in the firing step was 0.03%. After the obtained fired product was pulverized, coarse particles and fine particles were removed using a sieve to obtain Mn ferrite particles having an average particle diameter of 45 μm.
The surface roughness, saturation magnetization σs, chargeability, and X-ray diffraction of the obtained ferrite particles were measured in the same manner as in Example 1. The results are shown in Table 1.

(比較例7)
Al粉を添加せず、焼成工程における焼成温度を1150℃とし、酸素濃度を0.03%とした以外は、実施例1と同様にして焼成物を得た。得られた焼成物を粉砕処理した後、篩を用いて粗粒及び微粒を除去し、平均粒子径45μmのMnフェライト粒子を得た。
得られたフェライト粒子の表面粗さ、飽和磁化σs、帯電性、X線回折を実施例1と同様にして測定した。結果を表1に示す。
(Comparative Example 7)
A fired product was obtained in the same manner as in Example 1 except that Al 2 O 3 powder was not added, the firing temperature in the firing step was 1150 ° C., and the oxygen concentration was 0.03%. After the obtained fired product was pulverized, coarse particles and fine particles were removed using a sieve to obtain Mn ferrite particles having an average particle diameter of 45 μm.
The surface roughness, saturation magnetization σs, chargeability, and X-ray diffraction of the obtained ferrite particles were measured in the same manner as in Example 1. The results are shown in Table 1.

(比較例8)
Al粉を添加せず、焼成工程における焼成温度を1200℃とし、酸素濃度を0.03%とした以外は、実施例1と同様にして焼成物を得た。得られた焼成物を粉砕処理した後、篩を用いて粗粒及び微粒を除去し、平均粒子径45μmのMnフェライト粒子を得た。
得られたフェライト粒子の表面粗さ、飽和磁化σs、帯電性、X線回折を実施例1と同様にして測定した。結果を表1に示す。
(Comparative Example 8)
A fired product was obtained in the same manner as in Example 1 except that Al 2 O 3 powder was not added, the firing temperature in the firing step was 1200 ° C., and the oxygen concentration was 0.03%. After the obtained fired product was pulverized, coarse particles and fine particles were removed using a sieve to obtain Mn ferrite particles having an average particle diameter of 45 μm.
The surface roughness, saturation magnetization σs, chargeability, and X-ray diffraction of the obtained ferrite particles were measured in the same manner as in Example 1. The results are shown in Table 1.

帯電ムラの評価として、図3における実施例3の帯電レベル(最大値−最小値の差)を1とした時、1.5までを「小」、1.5以上を「大」と定めた。表1から明らかなように、実施例1〜6の本発明に係るフェライト粒子では、帯電ムラはいずれも小さかった。   As the evaluation of charging unevenness, when the charging level (difference between maximum value and minimum value) of Example 3 in FIG. 3 is 1, 1.5 is defined as “small”, and 1.5 or more is defined as “large”. . As is apparent from Table 1, the ferrite particles according to the present invention in Examples 1 to 6 had small charging unevenness.

また、粉砕前後でXRD測定ピーク強度差が小さく、FeとMnFeの組成比率が表面と内部で均一であることを示している。よって、粒子表面の摩耗や欠けによって生じる、電気抵抗の変動・低下する不具合を低減させることができる。 Moreover, the XRD measurement peak intensity difference is small before and after the pulverization, indicating that the composition ratio of Fe 2 O 3 and MnFe 2 O 4 is uniform between the surface and the inside. Therefore, it is possible to reduce a problem that electric resistance fluctuates or decreases due to wear or chipping on the particle surface.

本発明に係る磁気ブラシ帯電用のフェライト粒子によれば、長期間使用しても電気抵抗が変動・低下することなく、また安定した帯電性が得られ有用である。   The ferrite particles for charging a magnetic brush according to the present invention are useful because the electrical resistance does not fluctuate or decrease even when used for a long period of time, and a stable charging property is obtained.

1 磁気ブラシ帯電装置
2 感光体ドラム
3 電圧印加電源
11 磁気スリーブ
12 マグネットロール
13 磁性粒子
DESCRIPTION OF SYMBOLS 1 Magnetic brush charging device 2 Photosensitive drum 3 Voltage supply power source 11 Magnetic sleeve 12 Magnet roll 13 Magnetic particle

Claims (5)

一般式MnFe3−x(但し、0≦x≦1)で表される材料を主成分とし、磁気ブラシ帯電に用いられるフェライト粒子であって、
粒子の表面粗さが0.4〜0.6μmの範囲で、飽和磁化が60emu/g以上であり、
X線回折で得られるFeとMnFeとのピーク強度比の、粉砕前と粉砕後の差が絶対値で0.015以下であることを特徴とするフェライト粒子。
Formula Mn x Fe 3-x O 4 ( where, 0 ≦ x ≦ 1) as a main component a material represented by a ferrite particles used in the magnetic brush charging,
The surface roughness of the particles is in the range of 0.4 to 0.6 μm, the saturation magnetization is 60 emu / g or more,
A ferrite particle characterized in that the difference between the peak intensity ratio of Fe 2 O 3 and MnFe 2 O 4 obtained by X-ray diffraction before and after pulverization is 0.015 or less in absolute value.
Alが、Al換算で0.2〜2.0重量%の固溶している請求項1記載のフェライト粒子。   The ferrite particle according to claim 1, wherein Al is dissolved in an amount of 0.2 to 2.0 wt% in terms of Al. 印加電圧1000Vのときの電気抵抗値が1.0×10〜9.0×10Ωの範囲である請求項1又は2記載のフェライト粒子。 3. The ferrite particle according to claim 1, wherein an electric resistance value at an applied voltage of 1000 V is in a range of 1.0 × 10 6 to 9.0 × 10 8 Ω. 一般式MnFe3−x(但し、0≦x≦1)で表わされる組成のフェライト粒子が生成するように成分調整されたFe原料とMn原料、及びAl原料を媒体液中で混合してスラリーを得る工程と、前記スラリーを噴霧乾燥させて造粒物を得る工程と、酸素濃度が1.0〜1.7%の範囲で前記造粒物を焼成して焼成物を得る工程とを有することを特徴とする磁気ブラシ帯電用のフェライト粒子の製造方法。 Mixing Fe raw material, Mn raw material, and Al raw material, which are component-adjusted so that ferrite particles having a composition represented by the general formula Mn x Fe 3-x O 4 (where 0 ≦ x ≦ 1) are generated, are mixed in the medium liquid. And obtaining a slurry by spray drying the slurry to obtain a granulated product, and firing the granulated product in an oxygen concentration range of 1.0 to 1.7% to obtain a calcined product. And a method for producing ferrite particles for charging a magnetic brush. Al原料の添加量が、Al換算で0.2〜2.0重量%の範囲である請求項4記載のフェライト粒子の製造方法。   The method for producing ferrite particles according to claim 4, wherein the additive amount of the Al raw material is in the range of 0.2 to 2.0% by weight in terms of Al.
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