TWI667220B - MnCoZn ferrite and manufacturing method thereof - Google Patents

MnCoZn ferrite and manufacturing method thereof Download PDF

Info

Publication number
TWI667220B
TWI667220B TW107120211A TW107120211A TWI667220B TW I667220 B TWI667220 B TW I667220B TW 107120211 A TW107120211 A TW 107120211A TW 107120211 A TW107120211 A TW 107120211A TW I667220 B TWI667220 B TW I667220B
Authority
TW
Taiwan
Prior art keywords
mncozn
less
mol
mass ppm
ferrite
Prior art date
Application number
TW107120211A
Other languages
Chinese (zh)
Other versions
TW201912609A (en
Inventor
吉田裕史
中村由紀子
Original Assignee
日商杰富意化學股份有限公司
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by 日商杰富意化學股份有限公司 filed Critical 日商杰富意化學股份有限公司
Publication of TW201912609A publication Critical patent/TW201912609A/en
Application granted granted Critical
Publication of TWI667220B publication Critical patent/TWI667220B/en

Links

Classifications

    • CCHEMISTRY; METALLURGY
    • C01INORGANIC CHEMISTRY
    • C01GCOMPOUNDS CONTAINING METALS NOT COVERED BY SUBCLASSES C01D OR C01F
    • C01G49/00Compounds of iron
    • CCHEMISTRY; METALLURGY
    • C04CEMENTS; CONCRETE; ARTIFICIAL STONE; CERAMICS; REFRACTORIES
    • C04BLIME, MAGNESIA; SLAG; CEMENTS; COMPOSITIONS THEREOF, e.g. MORTARS, CONCRETE OR LIKE BUILDING MATERIALS; ARTIFICIAL STONE; CERAMICS; REFRACTORIES; TREATMENT OF NATURAL STONE
    • C04B35/00Shaped ceramic products characterised by their composition; Ceramics compositions; Processing powders of inorganic compounds preparatory to the manufacturing of ceramic products
    • C04B35/622Forming processes; Processing powders of inorganic compounds preparatory to the manufacturing of ceramic products
    • C04B35/626Preparing or treating the powders individually or as batches ; preparing or treating macroscopic reinforcing agents for ceramic products, e.g. fibres; mechanical aspects section B
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F1/00Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
    • H01F1/01Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
    • H01F1/03Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
    • H01F1/12Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials
    • H01F1/34Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of soft-magnetic materials non-metallic substances, e.g. ferrites
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F41/00Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties
    • H01F41/02Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for manufacturing cores, coils, or magnets

Landscapes

  • Chemical & Material Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Manufacturing & Machinery (AREA)
  • Organic Chemistry (AREA)
  • Inorganic Chemistry (AREA)
  • Ceramic Engineering (AREA)
  • Dispersion Chemistry (AREA)
  • Materials Engineering (AREA)
  • Structural Engineering (AREA)
  • Magnetic Ceramics (AREA)
  • Soft Magnetic Materials (AREA)

Abstract

本發明提供一種MnCoZn鐵氧體,其為如下MnCoZn系鐵氧體,作為基本成分,包含鐵:以Fe2O3換算計為45.0mol%以上且未滿50.0mol%、鋅:以ZnO換算計為15.5mol%~24.0mol%、鈷:以CoO換算計為0.5mol%~4.0mol%及錳:剩餘部分,相對於所述基本成分而言,作為副成分,包含SiO2:50massppm~300massppm及CaO:300massppm~1300massppm,且剩餘部分包含不可避免的雜質,將所述不可避免的雜質中的P、B、S及Cl量分別抑制為P:未滿50massppm、B:未滿20massppm、S:未滿30massppm及Cl:未滿50massppm,進而,將磨耗值設為未滿0.85%,將23℃下的方形比設為0.35以下,將比電阻設為30Ω.m以上,以及將居里溫度設為100℃以上。 The present invention provides a MnCoZn ferrite which is a MnCoZn ferrite as a basic component and contains iron: 45.0 mol% or more and less than 50.0 mol% in terms of Fe 2 O 3 , and zinc: in terms of ZnO 15.5 mol% to 24.0 mol%, cobalt: 0.5 mol% to 4.0 mol% in terms of CoO, and manganese: the remainder, containing SiO 2 : 50 mass ppm to 300 mass ppm as a subcomponent with respect to the basic component CaO: 300 mass ppm to 1300 mass ppm, and the remainder contains unavoidable impurities, and the amounts of P, B, S, and Cl in the unavoidable impurities are respectively suppressed to P: less than 50 mass ppm, B: less than 20 mass ppm, S: not 30massppm and Cl: less than 50massppm, further, the wear value is less than 0.85%, the square ratio at 23°C is set to 0.35 or less, and the specific resistance is set to 30Ω. m or more, and the Curie temperature is set to 100 ° C or more.

Description

MnCoZn系鐵氧體及其製造方法 MnCoZn ferrite and manufacturing method thereof

本發明是有關於一種比電阻高、作為殘留磁通量密度相對於飽和磁通量密度之比(殘留磁通量密度/飽和磁通量密度)的方形比小、且不易缺損的MnCoZn系鐵氧體及其製造方法。 The present invention relates to a MnCoZn-based ferrite having a high specific resistance, a square ratio which is a ratio of a residual magnetic flux density to a saturation magnetic flux density (residual magnetic flux density/saturated magnetic flux density), and which is less likely to be defective, and a method for producing the same.

再者,本說明書中,方形比是指23℃下的值。 Further, in the present specification, the square ratio means a value at 23 °C.

作為軟磁性氧化物磁性材料的代表性例子,可列舉MnZn鐵氧體。現有的MnZn鐵氧體包含約2質量%(mass%)以上的具有正磁各向異性的Fe2+,藉由使其與具有負磁各向異性的Fe3+、Mn2+抵消,而於kHz區域達成高的初透磁率或低損失。 A representative example of the soft magnetic oxide magnetic material is MnZn ferrite. The conventional MnZn ferrite contains about 2 mass% (mass%) or more of Fe 2+ having positive magnetic anisotropy, which is offset by Fe 3+ and Mn 2+ having negative magnetic anisotropy. A high initial permeability or low loss is achieved in the kHz region.

與非晶質金屬等比較而言,該MnZn鐵氧體廉價,因此被廣泛用作開關電源等的雜訊濾波器(noise filter)或變壓器(transformer)或天線的磁心。 Since the MnZn ferrite is inexpensive compared with an amorphous metal or the like, it is widely used as a noise filter such as a switching power supply, a transformer, or a core of an antenna.

但是,MnZn鐵氧體由於Fe2+量多,因此有容易引起Fe3+-Fe2+間的電子傳遞,且比電阻低至0.1Ω.m級別的缺點。因此,若所使用的頻率區域變高,則由在鐵氧體內流動的渦流所引起的損失劇增,初透磁率大大降低,損失亦增大。因此,MnZn鐵氧體的耐用頻率的極限為數百kHz左右,於MHz級別主要使用NiZn鐵氧體。該NiZn鐵氧體的比電阻為105(Ω.m)以上,且為 MnZn鐵氧體的約1萬倍,渦流損失少,因此即便於高頻區域,亦不易失去高初透磁率、低損失這一特性。 However, since MnZn ferrite has a large amount of Fe 2+ , it is easy to cause electron transfer between Fe 3+ -Fe 2+ and the specific resistance is as low as 0.1 Ω. The disadvantage of the m level. Therefore, if the frequency region to be used becomes high, the loss caused by the eddy current flowing in the ferrite body sharply increases, the initial permeability is greatly lowered, and the loss is also increased. Therefore, the limit of the durability frequency of the MnZn ferrite is about several hundred kHz, and NiZn ferrite is mainly used at the MHz level. The NiZn ferrite has a specific resistance of 10 5 (Ω·m) or more, and is about 10,000 times that of the MnZn ferrite, and has a small eddy current loss. Therefore, even in a high frequency region, it is difficult to lose high initial permeability and low. Loss of this feature.

但是,NiZn鐵氧體中存在大的問題點。其為:較Mn而言,Ni的負磁各向異性能量大,並且幾乎不含具有正磁各向異性的Fe2+,因此方形比變大。所謂方形比,是將殘留磁通量密度除以飽和磁通量密度所得者,於該值大的情況下,暫時自外部施加了磁場之後,初透磁率大大降低,同時導致損失的增大。因此,大大損害作為軟磁性材料的特性。 However, there are big problems in NiZn ferrite. It is that, compared with Mn, Ni has a large negative magnetic anisotropy energy and contains almost no Fe 2+ having positive magnetic anisotropy, so the square ratio becomes large. The square ratio is obtained by dividing the residual magnetic flux density by the saturation magnetic flux density. When the value is large, after the magnetic field is temporarily applied from the outside, the initial permeability is greatly lowered and the loss is increased. Therefore, the characteristics as a soft magnetic material are greatly impaired.

作為除NiZn鐵氧體以外獲得比電阻大的鐵氧體的方法,有如下方法:藉由減少MnZn鐵氧體中所含的Fe2+量而使比電阻上升。 As a method of obtaining a ferrite having a larger specific resistance than NiZn ferrite, there is a method of increasing the specific resistance by reducing the amount of Fe 2+ contained in the MnZn ferrite.

例如,於專利文獻1、專利文獻2及專利文獻3等中,報告有一種藉由將Fe2O3成分設為未滿50mol%並減少Fe2+含量而提高了比電阻的MnZn鐵氧體。但是,該些與NiZn鐵氧體同樣,亦僅包含具有負磁各向異性的離子,因此,完全未解決方形比的降低這一課題。 For example, in Patent Document 1, Patent Document 2, and Patent Document 3, there is reported a MnZn ferrite having improved specific resistance by setting the Fe 2 O 3 component to less than 50 mol% and reducing the Fe 2+ content. . However, like these NiZn ferrites, since only ions having negative magnetic anisotropy are contained, the problem of lowering the square ratio is not solved at all.

因此,於專利文獻4、專利文獻5及專利文獻6中揭示有一種添加除Fe2+以外的具有正磁各向異性的Co2+的技術,但該些並未將方形比的降低作為目的。另外,針對後述異常粒子的對策並不充分,因此,於成本及製造效率的方面亦差。 For this reason, Patent Document 4, Patent Document 5, and Patent Document 6 disclose a technique of adding Co 2+ having positive magnetic anisotropy other than Fe 2+ , but these do not have a purpose of reducing the square ratio. . In addition, countermeasures against abnormal particles described later are not sufficient, and therefore, they are also inferior in terms of cost and manufacturing efficiency.

相對於此,專利文獻7中報告有一種藉由對雜質組成設置規定來抑制異常粒子的出現、可實現穩定製造、且方形比低的 高電阻MnCoZn鐵氧體。 On the other hand, Patent Document 7 reports that the provision of an impurity composition is set to suppress the occurrence of abnormal particles, stable manufacturing can be achieved, and the square ratio is low. High resistance MnCoZn ferrite.

再者,所謂異常粒子生長,是因某些原因而粒子生長的平衡局部崩潰時所發生者,是於使用粉末冶金法進行製造時經常見到的現象。於該異常生長粒子內混入雜質或晶格缺陷等大大妨礙磁壁移動的物質,因此,殘留磁通量密度上升,其結果,方形比上升。同時,晶界形成變得不充分,因此比電阻降低。 Further, the abnormal particle growth is a phenomenon which occurs when the balance of particle growth locally collapses for some reason, and is a phenomenon often seen when manufacturing by the powder metallurgy method. A substance that greatly hinders the movement of the magnetic wall is contaminated with impurities or lattice defects in the abnormally grown particles. Therefore, the residual magnetic flux density increases, and as a result, the square ratio increases. At the same time, the grain boundary formation becomes insufficient, and thus the specific resistance is lowered.

[現有技術文獻] [Prior Art Literature] [專利文獻] [Patent Literature]

專利文獻1:日本專利特開平7-230909號公報 Patent Document 1: Japanese Patent Laid-Open No. Hei 7-230909

專利文獻2:日本專利特開2000-277316號公報 Patent Document 2: Japanese Patent Laid-Open Publication No. 2000-277316

專利文獻3:日本專利特開2001-220222號公報 Patent Document 3: Japanese Patent Laid-Open Publication No. 2001-220222

專利文獻4:日本專利第3418827號公報 Patent Document 4: Japanese Patent No. 3418827

專利文獻5:日本專利特開2001-220221公報 Patent Document 5: Japanese Patent Laid-Open Publication No. 2001-220221

專利文獻6:日本專利特開2001-68325號公報 Patent Document 6: Japanese Patent Laid-Open Publication No. 2001-68325

專利文獻7:日本專利4508626號公報 Patent Document 7: Japanese Patent No. 4508626

專利文獻8:日本專利特開2006-44971號公報 Patent Document 8: Japanese Patent Laid-Open No. 2006-44971

藉由所述專利文獻7的開發,獲得了滿足磁特性的MnCoZn鐵氧體。 With the development of Patent Document 7, MnCoZn ferrite which satisfies magnetic properties is obtained.

另一方面,近年來汽車的電裝化的趨勢顯著,MnCoZn鐵氧體亦被搭載於汽車中的情形增多,但於該用途中受到重視的特性 為機械強度。與迄今為止作為主要用途的電氣製品或產業用機器比較,於汽車中,移行時會產生震動,因此於車載用途中,對作為陶瓷的MnCoZn鐵氧體亦要求相對於震動的衝擊而言無缺損者。 On the other hand, in recent years, the trend of electrification of automobiles has become remarkable, and MnCoZn ferrites have been installed in automobiles, but they have received attention in this application. For mechanical strength. Compared with electrical equipment or industrial equipment that has been used as a main purpose so far, vibration occurs during traveling in automobiles. Therefore, in automotive applications, MnCoZn ferrite as ceramic is required to have no damage with respect to shock. By.

但是,Fe2O3成分未滿50mol%的MnCoZn鐵氧體由於氧孔隙少,因此,煅燒時容易進行燒結,因此,容易於晶粒內殘存孔隙,且晶界的生成容易變得不均勻。其結果,於受到來自外部的衝擊的情況下,與現有的MnCoZn鐵氧體比較,存在容易發生缺損的問題。 However, since the MnCoZn ferrite having a Fe 2 O 3 component of less than 50 mol% has a small amount of oxygen pores, it is easy to be sintered at the time of firing. Therefore, pores are likely to remain in the crystal grains, and formation of grain boundaries is likely to be uneven. As a result, when subjected to an impact from the outside, there is a problem that the defect is likely to occur as compared with the conventional MnCoZn ferrite.

即,專利文獻7所揭示的技術中,所獲得的磁特性充分,另一方面,關於針對該缺損的機械強度,於未必充分之處殘留有問題。 That is, in the technique disclosed in Patent Document 7, the obtained magnetic characteristics are sufficient, and on the other hand, there is a problem that the mechanical strength against the defect is not sufficient.

再者,作為改善缺損強度的技術,專利文獻8中已知有於0.01mass%~0.5mass%的範圍內添加TiO2的技術。 Further, as a technique for improving the defect strength, Patent Document 8 discloses a technique of adding TiO 2 in a range of 0.01 mass% to 0.5 mass%.

然而,關於TiO2的添加,另一方面,由於固溶於晶粒內並生成Ti4+,且自價數平衡起一部分Fe3+被還原為Fe2+,因此有導致比電阻大幅度降低的不利之處。 However, regarding the addition of TiO 2 , on the other hand, since solid solution is dissolved in the crystal grains and Ti 4+ is formed , and a part of Fe 3+ is reduced to Fe 2+ from the valence balance, the specific resistance is greatly lowered. The disadvantages.

本發明的目的在於一併提出如下MnCoZn鐵氧體及其有利的製造方法,所述MnCoZn鐵氧體保持現有的高電阻、低方形比這一良好的磁特性,並且藉由與生成均勻的晶界同時地抑制異常粒子生長而亦兼具由磨耗值表示的耐缺損性這一機械強度。 The object of the present invention is to jointly propose a MnCoZn ferrite which maintains the good magnetic properties of the existing high resistance and low square ratio, and an advantageous manufacturing method thereof, and which generates uniform crystals by The boundary suppresses the growth of abnormal particles at the same time, and also has the mechanical strength of the defect resistance represented by the wear value.

發明者等人首先針對為了獲得所期望的磁特性而需要 的MnCoZn鐵氧體的Fe2O3、ZnO、及CoO的合理量進行了研究,結果發現了可同時實現比電阻高、方形比小、且居里溫度高這些全部特性的合理範圍。 The inventors first studied the reasonable amount of Fe 2 O 3 , ZnO, and CoO of MnCoZn ferrite required to obtain desired magnetic properties, and as a result, found that the specific resistance can be simultaneously achieved, and the square ratio is small. And a reasonable range of all the characteristics of high Curie temperature.

再者,本說明書中,如所述般,關於方形比,將23℃下的值作為問題。即為,於天線或雜訊濾波器的用途中所使用的MnZn鐵氧體磁心(ferrite core)中,亦有許多於遠離成為熱源的電源變壓器或半導體的位置使用者,該些於常溫(5℃~35℃)下進行運轉。因此,重要的是作為常溫(5℃~35℃)範圍的代表值的23℃下的磁特性良好,即,方形比小。 Further, in the present specification, as described above, the value at 23 ° C is a problem with respect to the square ratio. That is, in the MnZn ferrite core used in the use of an antenna or a noise filter, there are also many users who are away from the power transformer or semiconductor that is a heat source, and these are at normal temperature (5). Operate at °C~35°C). Therefore, it is important that the magnetic characteristics at 23 ° C which is a representative value in the range of normal temperature (5 ° C to 35 ° C) are good, that is, the square ratio is small.

繼而,著眼於微細組織,發現藉由減少晶粒內的孔隙、調整結晶粒度且實現適度的厚度的粒界,可抑制由磨耗值表示的燒結磁心的缺損。此處,為了實現所期望的結晶組織,由於作為於晶界偏析的成分的SiO2及CaO的添加量產生大的影響,因此成功確定了該些成分的適量範圍。若為該範圍內,則可保持低磨耗值。 Then, focusing on the fine structure, it was found that the defect of the sintered core represented by the wear value can be suppressed by reducing the voids in the crystal grains, adjusting the crystal grain size, and realizing a grain boundary of a moderate thickness. Here, in order to realize a desired crystal structure, since the amount of SiO 2 and CaO added as a component segregated at the grain boundary has a large influence, the appropriate range of the components is successfully determined. If it is within this range, the low wear value can be maintained.

進而,關於為了併有較佳的磁特性及針對缺損的機械強度而不可或缺的對異常粒子出現的抑制,著眼於異常粒子出現時的製作條件而進行了研究,結果發現,於所述SiO2及CaO過多的情況下,以及於含有某一定值以上的作為源於原料的雜質的P、B、S及Cl等成分的情況下,異常粒子出現。 Further, in order to suppress the occurrence of abnormal particles in order to have better magnetic properties and mechanical strength against defects, attention has been paid to the production conditions at the time of occurrence of abnormal particles, and it has been found that the SiO is found. When the amount of CaO is too large, and when a component such as P, B, S or Cl which is a source-derived impurity containing a certain value or more is contained, abnormal particles appear.

本發明是立足於所述見解而成者。 The present invention is based on the insights.

再者,上文中已進行了敘述,於專利文獻1、專利文獻 2及專利文獻3等中,關於高比電阻,已有所提及,另外,於專利文獻4、專利文獻5及專利文獻6中,關於具有正磁各向異性的Co2+的添加,已進行了敘述,但並無與方形比有關的記載,且完全沒有關於異常粒子對策的記載,因此推測機械強度亦不充分。另外,關於提及了低方形比的專利文獻7,由於添加物的規定不充分,因此無法期望能夠抑制缺損的充分的機械強度。進而,即便是提及了缺損強度的改善的專利文獻8,亦無法避免比電阻的大幅度降低。 In addition, in the above-mentioned patent document 1, the patent document 2, the patent document 3, etc., about high specific resistance, it is mentioned, and patent document 4, patent document 5, and patent document 6 Although the addition of Co 2+ having positive magnetic anisotropy has been described, there is no description about the square ratio, and there is no description about the countermeasure against abnormal particles at all. Therefore, it is estimated that the mechanical strength is also insufficient. Further, in Patent Document 7 in which the low square ratio is mentioned, since the regulation of the additive is insufficient, sufficient mechanical strength capable of suppressing the defect cannot be expected. Further, even in Patent Document 8 which mentions an improvement in defect strength, a large reduction in specific resistance cannot be avoided.

本發明的主旨構成如下所述。 The gist of the present invention is as follows.

1.一種MnCoZn系鐵氧體,其中,作為基本成分,包含鐵:以Fe2O3換算計為45.0mol%以上且未滿50.0mol%、鋅:以ZnO換算計為15.5mol%~24.0mol%、鈷:以CoO換算計為0.5mol%~4.0mol%及錳:剩餘部分,相對於所述基本成分而言,作為副成分,包含SiO2:50massppm~300massppm及CaO:300massppm~1300massppm,且剩餘部分包含不可避免的雜質,將所述不可避免的雜質中的P、B、S及Cl量分別抑制為P:未滿50massppm、B:未滿20massppm、 S:未滿30massppm及Cl:未滿50massppm,進而,於所述MnCoZn系鐵氧體中,磨耗值未滿0.85%,23℃下的方形比為0.35以下,比電阻為30Ω.m以上,以及居里溫度為100℃以上。 1. A MnCoZn-based ferrite containing, as a basic component, iron: 45.0 mol% or more and less than 50.0 mol% in terms of Fe 2 O 3 and zinc: 15.5 mol% to 24.0 mol in terms of ZnO %, cobalt: 0.5 mol% to 4.0 mol% in terms of CoO and manganese: the remainder, as the subcomponent, includes SiO 2 : 50 mass ppm to 300 mass ppm and CaO: 300 mass ppm to 1300 mass ppm, and The remaining portion contains unavoidable impurities, and the amounts of P, B, S, and Cl in the unavoidable impurities are respectively suppressed to P: less than 50 mass ppm, B: less than 20 mass ppm, S: less than 30 mass ppm, and Cl: less than 50 mass ppm, further, in the MnCoZn ferrite, the abrasion value is less than 0.85%, the square ratio at 23 ° C is 0.35 or less, and the specific resistance is 30 Ω. m or more, and the Curie temperature is 100 ° C or more.

2.如所述1所述的MnCoZn系鐵氧體,其中,所述MnCoZn系鐵氧體的燒結密度為4.85g/cm3以上。 2. The MnCoZn-based ferrite according to 1, wherein the MnCoZn-based ferrite has a sintered density of 4.85 g/cm 3 or more.

3.如所述1或2所述的MnCoZn系鐵氧體,其中,所述MnCoZn系鐵氧體為包含粒度分佈d90的值為300μm以下的造粒粉的成形-燒結體的MnCoZn系鐵氧體。 3. The MnCoZn-based ferrite according to the above-mentioned item 1 or 2, wherein the MnCoZn-based ferrite is a MnCoZn-based ferrite of a formed-sintered body containing a granulated powder having a particle size distribution d90 of 300 μm or less. body.

4.如所述1至3中任一項所述的MnCoZn系鐵氧體,其中,所述MnCoZn系鐵氧體為包含壓碎強度未滿1.50MPa的造粒粉的成形-燒結體的MnCoZn系鐵氧體。 The MnCoZn-based ferrite according to any one of the above-mentioned, wherein the MnCoZn-based ferrite is a shaped-sintered MnCoZn containing a granulated powder having a crushing strength of less than 1.50 MPa. Ferrite.

5.一種MnCoZn系鐵氧體的製造方法,其包括:預煅燒步驟,對以成為規定的成分比率的方式秤量的基本成分的混合物進行預煅燒;混合-粉碎步驟,向所述預煅燒步驟中所得的預煅燒粉中添加已調整為規定比率的副成分,並加以混合、粉碎;以及煅燒步驟,向所述混合-粉碎步驟中所得的粉碎粉中添加黏合劑並加以混合後,以造粒粉的粒度分佈d90的值成為300μm以下 及/或壓碎強度未滿1.50MPa的方式進行造粒,並將所得的造粒粉加以成形後,於最高保持溫度:1290℃以上、保持時間:1小時以上的條件下進行煅燒,從而獲得如所述1或2所述的MnCoZn系鐵氧體。 A method for producing a MnCoZn-based ferrite, comprising: a pre-calcining step of pre-calcining a mixture of basic components weighed so as to have a predetermined component ratio; and a mixing-pulverizing step to the pre-calcining step To the obtained pre-calcined powder, an auxiliary component adjusted to a predetermined ratio is added, mixed and pulverized; and a calcination step, a binder is added to the pulverized powder obtained in the mixing-pulverizing step, and mixed, and then granulated The value of the particle size distribution d90 of the powder is 300 μm or less. And/or granulation is carried out so that the crushing strength is less than 1.50 MPa, and the obtained granulated powder is molded, and then calcined under the conditions of a maximum holding temperature: 1290 ° C or more and a holding time: 1 hour or more. The MnCoZn-based ferrite according to the above 1 or 2.

6.如所述5所述的MnCoZn系鐵氧體的製造方法,其中,所述造粒為噴霧乾燥法。 6. The method for producing a MnCoZn-based ferrite according to the above 5, wherein the granulation is a spray drying method.

根據本發明,可獲得如下MnCoZn鐵氧體,其不僅具有高電阻、低方形比這一良好的磁特性,而且藉由與生成均勻的晶界同時地抑制異常粒子生長而兼具優異的耐缺損性這一機械強度。 According to the present invention, the following MnCoZn ferrite can be obtained, which not only has good magnetic properties such as high electrical resistance and low square ratio, but also has excellent defect resistance by suppressing abnormal particle growth simultaneously with formation of uniform grain boundaries. This mechanical strength.

本發明的MnCoZn鐵氧體具有優異的磁特性:23℃、1kHz下的初透磁率為3000以上,23℃、1MHz下的初透磁率為2000以上,23℃、10MHz下的初透磁率為150以上。 The MnCoZn ferrite of the present invention has excellent magnetic properties: an initial permeability of 3,000 or more at 23 ° C and 1 kHz, an initial permeability of 2,000 or more at 23 ° C and 1 MHz, and an initial permeability of 150 at 23 ° C and 10 MHz. the above.

以下,對本發明進行具體說明。 Hereinafter, the present invention will be specifically described.

首先,對本發明中將MnCoZn鐵氧體的組成限定於所述範圍內的理由進行說明。再者,關於作為基本成分而包含於本發明中的鐵或鋅、鈷、錳,全部以換算為Fe2O3、ZnO、CoO、MnO的值來表示。另外,關於該些Fe2O3、ZnO、CoO、MnO的含量,以 mol%表示,另一方面,關於副成分及雜質成分的含量,以相對於鐵氧體整體的massppm表示。 First, the reason why the composition of the MnCoZn ferrite is limited to the above range in the present invention will be described. In addition, iron, zinc, cobalt, and manganese which are contained in the present invention as a basic component are all expressed by values of Fe 2 O 3 , ZnO, CoO, and MnO. In addition, the content of the Fe 2 O 3 , ZnO, CoO, and MnO is expressed by mol%, and the content of the subcomponent and the impurity component is represented by mass ppm with respect to the entire ferrite.

Fe2O3:45.0mol%~未滿50.0mol% Fe 2 O 3 : 45.0 mol% to less than 50.0 mol%

於過剩地包含Fe2O3的情況下,Fe2+量增加,藉此,MnCoZn鐵氧體的比電阻降低。為了避免該情況,需要將Fe2O3量抑制為未滿50mol%。但是,於Fe2O3量過少的情況下,導致方形比的上升及居里溫度的降低,因此,設為以Fe2O3換算計最少含有45.0mol%的鐵。較佳的Fe2O3的範圍為47.1mol%以上且未滿50.0mol%,更佳為47.1mol%~49.5mol%。 When Fe 2 O 3 is excessively contained, the amount of Fe 2+ is increased, whereby the specific resistance of the MnCoZn ferrite is lowered. In order to avoid this, it is necessary to suppress the amount of Fe 2 O 3 to less than 50 mol%. However, when the amount of Fe 2 O 3 is too small, the square ratio is increased and the Curie temperature is lowered. Therefore, it is required to contain at least 45.0 mol% of iron in terms of Fe 2 O 3 . The preferred range of Fe 2 O 3 is 47.1 mol% or more and less than 50.0 mol%, more preferably 47.1 mol% to 49.5 mol%.

ZnO:15.5mol%~24.0mol% ZnO: 15.5 mol% to 24.0 mol%

ZnO由於使鐵氧體的飽和磁化增加,並且飽和蒸氣壓比較低,因此具有使燒結密度上升且使飽和磁通量密度上升的作用,且為對於方形比的降低而言有效的成分。因此,設為以ZnO換算計最少含有15.5mol%的鋅。另一方面,於鋅含量較合理的值多的情況下,導致居里溫度降低,於實用上有問題。因此,以ZnO換算計將鋅的上限設為24.0mol%。較佳為的ZnO的範圍為15.5mol%~23.0mol%,更佳為17.0mol%~23.0mol%。 Since ZnO increases the saturation magnetization of the ferrite and has a relatively low saturated vapor pressure, it has a function of increasing the sintered density and increasing the saturation magnetic flux density, and is a component effective for reducing the square ratio. Therefore, it is assumed that at least 15.5 mol% of zinc is contained in terms of ZnO. On the other hand, in the case where the zinc content is more than a reasonable value, the Curie temperature is lowered, which is problematic in practical use. Therefore, the upper limit of zinc is set to 24.0 mol% in terms of ZnO. The range of ZnO is preferably 15.5 mol% to 23.0 mol%, more preferably 17.0 mol% to 23.0 mol%.

CoO:0.5mol%~4.0mol% CoO: 0.5 mol% to 4.0 mol%

CoO中的Co2+為具有正磁各向異性能量的離子,伴隨該CoO的合理量的添加,磁各向異性能量的總和的絕對值降低,結果實現方形比的降低。因此必須添加0.5mol%以上的CoO。另一方面,大量的添加由於比電阻的降低、異常粒子生長的引發、且磁各向 異性能量的總和過度傾向於正,反而導致方形比的上升。為了防止該情況,設為使CoO止於最多添加4.0mol%。較佳的CoO的範圍為1.0mol%~3.5mol%,更佳為1.0mol%~3.0mol%。 Co 2+ in CoO is an ion having positive magnetic anisotropy energy, and with the addition of a reasonable amount of CoO, the absolute value of the sum of magnetic anisotropy energy is lowered, and as a result, the square ratio is lowered. Therefore, it is necessary to add 0.5 mol% or more of CoO. On the other hand, a large amount of addition causes a square ratio to rise due to a decrease in specific resistance, an initiation of abnormal particle growth, and an excessively large sum of magnetic anisotropy energy. In order to prevent this, it is assumed that CoO is stopped at a maximum of 4.0 mol%. A preferred range of CoO is from 1.0 mol% to 3.5 mol%, more preferably from 1.0 mol% to 3.0 mol%.

MnO:剩餘部分 MnO: the remaining part

本發明為MnCoZn鐵氧體,基本成分組成的剩餘部分需要為MnO。其原因在於:若非MnO,則無法獲得高飽和磁通量密度、低損失及高透磁率的良好磁特性。較佳的MnO的範圍為26.5mol%~32.0mol%。 The present invention is a MnCoZn ferrite, and the remainder of the basic composition of the composition needs to be MnO. The reason for this is that if it is not MnO, good magnetic properties of high saturation magnetic flux density, low loss, and high magnetic permeability cannot be obtained. A preferred range of MnO is from 26.5 mol% to 32.0 mol%.

以上對基本成分進行了說明,關於副成分,如下所述。 The basic components have been described above, and the subcomponents are as follows.

SiO2:50massppm~300massppm SiO 2 : 50 mass ppm to 300 mass ppm

已知SiO2有助於鐵氧體的結晶組織的均勻化,伴隨適量的添加而減少殘留於晶粒內的孔隙,並使殘留磁通量密度降低,藉此使方形比降低。另外,SiO2藉由於粒界偏析而提高比電阻,同時使粗大粒徑的結晶減少,因此可降低作為燒結體的缺損指標的磨耗值。因此,設為最少含有50massppm的SiO2。另一方面,於添加量過多的情況下,反而會出現異常粒子,其成為缺損的起點,因此磨耗值上升,同時方形比亦上升,因此需要將SiO2的含有限制於300massppm以下。SiO2的較佳含量為60massppm~250massppm。 It is known that SiO 2 contributes to the homogenization of the crystal structure of the ferrite, and the pores remaining in the crystal grains are reduced with an appropriate amount of addition, and the residual magnetic flux density is lowered, whereby the square ratio is lowered. Further, since SiO 2 increases the specific resistance by segregation at the grain boundary and reduces the crystal of the coarse particle diameter, the wear value which is an index of the defect of the sintered body can be reduced. Therefore, it is assumed to contain at least 50 mass ppm of SiO 2 . On the other hand, when the amount of addition is too large, abnormal particles appear instead, and this becomes a starting point of the defect. Therefore, the abrasion value increases and the square ratio also increases. Therefore, it is necessary to limit the content of SiO 2 to 300 mass ppm or less. The preferred content of SiO 2 is from 60 mass ppm to 250 mass ppm.

CaO:300massppm~1300massppm CaO: 300 mass ppm to 1300 mass ppm

CaO具有於MnCoZn鐵氧體的晶界偏析並抑制晶粒生長的作用。因此,伴隨適量的添加而比電阻上升,且使殘留磁通量密度 降低,藉此,方形比亦降低,並且使粗大的結晶減少,因此亦能夠降低磨耗值。因此,設為最少含有300massppm的CaO。另一方面,於添加量過多的情況下出現異常粒子,且磨耗值及方形比亦上升,因此需要將CaO的含有限制於1300massppm以下。CaO的較佳含量為350massppm~1000massppm。 CaO has a role of segregating at the grain boundary of MnCoZn ferrite and suppressing grain growth. Therefore, the specific resistance increases with an appropriate amount of addition, and the residual magnetic flux density is made. By this, the square ratio is also lowered, and the coarse crystals are reduced, so that the abrasion value can also be lowered. Therefore, it is set to contain at least 300 mass ppm of CaO. On the other hand, when the amount of addition is too large, abnormal particles appear, and the wear value and the square ratio also increase. Therefore, it is necessary to limit the content of CaO to 1300 mass ppm or less. The preferred content of CaO is from 350 mass ppm to 1000 mass ppm.

繼而,對應加以抑制的雜質成分進行說明。 Next, the impurity component to be suppressed will be described.

P:未滿50massppm、B:未滿20massppm、S:未滿30massppm、以及Cl:未滿50massppm P: less than 50 mass ppm, B: less than 20 mass ppm, S: less than 30 mass ppm, and Cl: less than 50 mass ppm

該些為不可避免地包含於氧化鐵等原料中的成分。若該些的含有為極微量,則無問題,但於含有某一定以上的情況下,引發鐵氧體的異常粒子生長,並對所獲得的鐵氧體的各特性造成重大不良影響。如本發明般僅含有未滿50mol%的Fe2O3的組成的鐵氧體與含有50mol%以上者相比,容易進行結晶的粒子生長,因此,若P、B、S及Cl量多,則容易發生異常粒子生長。該情況下,伴隨殘留磁通量密度的上升而方形比上升,且晶界的生成變得不充分,因此比電阻降低,並成為缺損的起點,因此磨耗值亦上升。 These are components which are inevitably contained in raw materials such as iron oxide. If the content is extremely small, there is no problem. However, when a certain amount or more is contained, the abnormal particle growth of the ferrite is caused, and the characteristics of the obtained ferrite are seriously adversely affected. In the present invention, ferrite having a composition of only Fe 2 O 3 of less than 50 mol% is more likely to be crystallized than particles containing 50 mol% or more. Therefore, if the amounts of P, B, S, and Cl are large, Abnormal particle growth is prone to occur. In this case, the square ratio increases as the residual magnetic flux density increases, and the generation of grain boundaries becomes insufficient. Therefore, the specific resistance decreases and becomes a starting point of the defect, and thus the wear value also increases.

因此,本發明中,將P、B、S及Cl的含量分別抑制為未滿50massppm、未滿20massppm、未滿30massppm及未滿50massppm。 Therefore, in the present invention, the contents of P, B, S, and Cl are each suppressed to less than 50 mass ppm, less than 20 mass ppm, less than 30 mass ppm, and less than 50 mass ppm.

再者,需要將包含所述P、B、S及Cl在內的、不可避免的雜質的容許量整體設為70massppm以下。較佳為該不可避免的雜質的容許量為65massppm以下。 Further, it is necessary to set the total allowable amount of impurities including the P, B, S, and Cl to 70 mass ppm or less. It is preferable that the allowable amount of the unavoidable impurities is 65 mass ppm or less.

因而,較佳為極力抑制作為原材料而使用的基本成分及副成分中的雜質的混入。較佳為將作為原材料而使用的基本成分及副成分中的雜質的合計量包含所述P、B、S及Cl在內設為70massppm以下,更佳為設為65massppm以下。 Therefore, it is preferable to suppress the incorporation of impurities in the basic component and the subcomponent used as the raw material as much as possible. The total amount of the impurities in the basic component and the subcomponent used as the raw material is preferably 70 mass ppm or less, more preferably 65 mass ppm or less, including the P, B, S, and Cl.

另外,不限於組成,藉由各種參數而MnCoZn鐵氧體的各特性受到巨大影響。所以,本發明中為了具有所期望的磁特性、強度特性,較佳為滿足以下條件。 Further, not limited to the composition, various characteristics of the MnCoZn ferrite are greatly affected by various parameters. Therefore, in the present invention, in order to have desired magnetic properties and strength characteristics, the following conditions are preferably satisfied.

.燒結密度:4.85g/cm3以上 . Sintering density: 4.85g/cm 3 or more

MnCoZn鐵氧體藉由煅燒處理而進行燒結及粒子生長,從而構成晶粒及晶界。為了實現能夠實現高飽和磁通量密度及低殘留磁通量密度的結晶組織、即如下形態,需要充分地進行燒結反應,所述形態為:應存在於晶界的非磁性成分適當地於晶界偏析,晶粒包含保持適度的粒徑且具有均勻磁性的成分。另外,就缺損防止的觀點而言,於燒結不充分的情況下,強度亦降低,故欠佳。 The MnCoZn ferrite is sintered and subjected to particle growth by calcination treatment to form crystal grains and grain boundaries. In order to realize a crystal structure capable of realizing a high saturation magnetic flux density and a low residual magnetic flux density, that is, a form in which a non-magnetic component which is present at a grain boundary is appropriately segregated at a grain boundary, a crystal is required to be segregated. The granules contain ingredients that maintain a moderate particle size and have a uniform magnetic properties. Further, from the viewpoint of prevention of defects, when the sintering is insufficient, the strength is also lowered, which is not preferable.

就以上觀點而言,較佳為將本發明的MnCoZn鐵氧體的燒結密度設為4.85g/cm3以上。藉由滿足該條件,而方形比降低,且可將磨耗值抑制得低。再者,為了實現該燒結密度,需要將煅燒時的最高保持溫度設為1290℃以上,且以該溫度下的保持時間為1h以上進行煅燒。最高保持溫度較佳為1290℃~1400℃,保持時間較佳為1小時~8小時。另外,於發生了異常粒子生長的情況下燒結密度不會提高,因此,需要以不會出現異常粒子的方式,將上文所述的添加物量或雜質量控制於適當範圍內進行製作。 From the above viewpoints, the sintered density of the MnCoZn ferrite of the present invention is preferably 4.85 g/cm 3 or more. By satisfying this condition, the square ratio is lowered, and the abrasion value can be suppressed low. Further, in order to achieve the sintered density, it is necessary to set the maximum holding temperature at the time of firing to 1,290 ° C or higher, and to perform calcination at a holding time at this temperature of 1 h or more. The maximum holding temperature is preferably from 1290 ° C to 1400 ° C, and the holding time is preferably from 1 hour to 8 hours. Further, in the case where abnormal particle growth has occurred, the sintered density is not improved. Therefore, it is necessary to control the amount of the additive or the amount of impurities described above to an appropriate range so that the abnormal particles do not occur.

.使用粒度分佈d90的值為300μm以下的造粒粉進行製作。 . It is produced using a granulated powder having a particle size distribution d90 of 300 μm or less.

.使用造粒粉壓碎強度未滿1.50MPa的造粒粉進行製作。 . The granulated powder having a crushing strength of less than 1.50 MPa was used for the production.

一般而言,MnCoZn鐵氧體可藉由以下方式而獲得:經過將造粒粉填充於模具後以約100MPa的壓力進行壓縮的粉末成形步驟,對所獲得的成形體進行煅燒並使其燒結。由造粒粉彼此的間隙所引起的微小凹凸於燒結後亦殘存於該鐵氧體的表面,其成為相對於衝擊而言的缺損的起點,因此,伴隨微小凹凸的殘存的增加而磨耗值變高。因此,為了減少造粒粉彼此的間隙,較佳為將粒度粗的造粒粉去除且亦將造粒粉的壓碎強度抑制於一定值以下。 In general, the MnCoZn ferrite can be obtained by a powder forming step of compressing the granulated powder at a pressure of about 100 MPa after filling the mold, and the obtained shaped body is calcined and sintered. The minute irregularities caused by the gap between the granulated powders remain on the surface of the ferrite after sintering, and this is a starting point of the defect with respect to the impact. Therefore, the wear value changes as the residual of the fine unevenness increases. high. Therefore, in order to reduce the gap between the granulated powders, it is preferred to remove the granulated powder having a coarse particle size and also to suppress the crushing strength of the granulated powder to a certain value or less.

作為對於滿足所述條件而言有效的手段,關於粒度,有效的是藉由使所獲得的造粒粉通過篩來調整粒度。另一方面,為了使造粒粉的壓碎強度降低,有效的是當施加噴霧造粒法般的熱來造粒時,不使溫度變得過高。關於粒度分佈,藉由日本工業標準(Japanese Industrial Standards,JIS)Z 8825中記載的利用雷射繞射.散射法進行的粒徑分析來測定。所謂「d90」,表示粒度分佈曲線中的自小粒徑側起體積累計90%的粒徑。另外,對於造粒粉的壓碎強度,藉由JIS Z 8841中規定的方法來測定。 As means for satisfying the conditions, as for the particle size, it is effective to adjust the particle size by passing the obtained granulated powder through a sieve. On the other hand, in order to reduce the crushing strength of the granulated powder, it is effective to prevent the temperature from becoming too high when granulation is performed by applying heat like spray granulation. Regarding the particle size distribution, laser diffraction is described by Japanese Industrial Standards (JIS) Z 8825. The particle size analysis by the scattering method was carried out. The "d90" indicates a particle diameter of 90% cumulative from the small particle size side in the particle size distribution curve. Further, the crushing strength of the granulated powder was measured by the method specified in JIS Z 8841.

再者,若粒度分佈d90的值太小,則由於造粒粉間的接觸點的增加而導致流動性降低,因此出現粉體成形時的粉的模具填充的故障以及成形時的成形壓力增加的問題,故較佳為將d90的下 限設為75μm。另外,若造粒粉壓碎強度大大降低,則於輸送時以及粉的模具填充時造粒粉壓壞,流動性降低,藉此仍出現粉的模具填充時的故障以及成形時的成形壓力增加的問題,故較佳為將壓碎強度的下限設為0.50MPa。 In addition, if the value of the particle size distribution d90 is too small, the fluidity is lowered due to an increase in the contact point between the granulated powders, so that the mold filling failure of the powder during powder formation and the molding pressure at the time of molding increase occur. Problem, it is better to put under d90 The limit is set to 75 μm. In addition, if the crushing strength of the granulated powder is greatly lowered, the granulated powder is crushed at the time of conveyance and filling of the mold of the powder, and the fluidity is lowered, whereby the failure of the filling of the mold of the powder and the increase of the forming pressure at the time of molding still occur. Therefore, it is preferable to set the lower limit of the crushing strength to 0.50 MPa.

繼而,對本發明的MnCoZn鐵氧體的製造方法進行說明。 Next, a method for producing the MnCoZn ferrite of the present invention will be described.

關於MnCoZn鐵氧體的製造,首先以成為規定比率的方式秤量Fe2O3粉末、ZnO粉末、CoO粉末及MnO粉末,將該些充分混合後進行預煅燒。繼而將所獲得的預煅燒粉加以粉碎而獲得粉碎粉。此時,以規定的比率添加本發明中所規定的副成分,與預煅燒粉一併進行粉碎。該步驟中,以所添加的成分的濃度不偏頗的方式使粉末充分地均質化,同時使預煅燒粉微細化至目標平均粒徑的大小為止。此處,作為目標的粉碎粉的平均粒徑為1.4μm~1.0μm。 In the production of MnCoZn ferrite, first, Fe 2 O 3 powder, ZnO powder, CoO powder, and MnO powder are weighed so as to have a predetermined ratio, and these are sufficiently mixed and then pre-calcined. The obtained pre-calcined powder is then pulverized to obtain a pulverized powder. At this time, the subcomponents specified in the present invention are added at a predetermined ratio, and are pulverized together with the precalcined powder. In this step, the powder is sufficiently homogenized so that the concentration of the added component is not biased, and the pre-calcined powder is refined to a target average particle size. Here, the target pulverized powder has an average particle diameter of 1.4 μm to 1.0 μm.

繼而,向設為目標組成的粉末中添加聚乙烯醇等有機物黏合劑,為了獲得所期望的粒度及壓碎強度的試樣,於適當的條件下藉由利用噴霧乾燥法等的造粒來製成造粒粉。若為噴霧乾燥法,則理想的是使排風溫度低於270℃。此處,關於造粒粉的較佳粒度,粒度分佈d90的值為75μm~300μm。另外,造粒粉的較佳壓碎強度為0.50MPa以上且未滿1.50MPa。 Then, an organic binder such as polyvinyl alcohol is added to the powder having the target composition, and a sample having a desired particle size and crushing strength is obtained by granulation by a spray drying method or the like under appropriate conditions. Granulated into powder. In the case of the spray drying method, it is desirable to make the exhaust air temperature lower than 270 °C. Here, regarding the preferable particle size of the granulated powder, the value of the particle size distribution d90 is from 75 μm to 300 μm. Further, the preferred crushing strength of the granulated powder is 0.50 MPa or more and less than 1.50 MPa.

繼而,視需要經過用於粒度調整的過篩等步驟之後,於成形機中施加壓力並成形後,於適當的煅燒條件下進行煅燒。再者,理想的是於篩中使350μm的孔徑的造粒粉通過,並將篩上的粗粉 去除。另外,合理的煅燒條件是最高保持溫度為1290℃以上、保持時間為1小時以上。 Then, after passing through a step such as sieving for particle size adjustment, after applying pressure in a molding machine and forming, calcination is carried out under appropriate calcination conditions. Furthermore, it is desirable to pass a granulated powder having a pore size of 350 μm in the sieve and to coarsely powder the sieve. Remove. Further, a reasonable calcination condition is that the maximum holding temperature is 1290 ° C or higher and the holding time is 1 hour or longer.

再者,亦可對所獲得的鐵氧體燒結體實施表面研磨等加工。 Further, the obtained ferrite sintered body may be subjected to surface polishing or the like.

如此般,可獲得同時滿足先前不可能的、 In this way, it is possible to obtain both,

.磨耗值未滿0.85% . Wear value less than 0.85%

.23℃下的方形比為0.35以下 . The square ratio at 23 ° C is 0.35 or less

.比電阻為30Ω.m以上 . The specific resistance is 30Ω. m or more

.居里溫度為100℃以上、 . Curie temperature is above 100 °C,

的全部優異特性的、MnCoZn鐵氧體。 All of the excellent properties of MnCoZn ferrite.

[實施例] [Examples]

實施例1 Example 1

於將所包含的鐵、鋅、鈷及錳全部換算為Fe2O3、ZnO、CoO及MnO的情況下,使用球磨機將以Fe2O3、ZnO、CoO及MnO量成為表1所示比率的方式秤量的各原料粉末混合16小時後,於空氣中以925℃進行3小時預煅燒。繼而,分別秤量150massppm、700massppm相當量的SiO2、CaO後添加於該預煅燒粉中,利用球磨機粉碎12小時。繼而,向所獲得的粉碎漿料中添加聚乙烯醇,於排風溫度250℃下進行噴霧乾燥造粒,通過孔徑350μm的篩而將粗粉去除後,施加118MPa的壓力而成形為環形磁心(toroidal core)及長方體磁心。用於成形的造粒粉的粒度分佈d90為230μm,且壓碎強度為1.29MPa。 When all the iron, zinc, cobalt, and manganese contained are converted into Fe 2 O 3 , ZnO, CoO, and MnO, the ratios of Fe 2 O 3 , ZnO, CoO, and MnO are shown in Table 1 using a ball mill. Each of the raw material powders weighed was mixed for 16 hours, and then pre-calcined in air at 925 ° C for 3 hours. Then, SiO 2 and CaO in an amount of 150 mass ppm and 700 mass ppm were weighed and added to the pre-calcined powder, respectively, and pulverized by a ball mill for 12 hours. Then, polyvinyl alcohol was added to the obtained pulverized slurry, spray-dried and granulated at an exhaust air temperature of 250 ° C, and the coarse powder was removed by a sieve having a pore size of 350 μm, and then a pressure of 118 MPa was applied to form a toroidal core ( Toroidal core) and cuboid core. The granulated powder for forming had a particle size distribution d90 of 230 μm and a crush strength of 1.29 MPa.

其後,將該成形體放入煅燒爐中,於最高溫度1350℃下,於 將氮氣與空氣適宜混合而成的氣流中煅燒2小時,獲得外徑:25mm、內徑:15mm、高度:5mm的燒結體環形磁心、與5個直徑:10mm、高度:10mm的燒結體圓柱形狀磁心。 Thereafter, the shaped body is placed in a calciner at a maximum temperature of 1,350 ° C, Calcined in a gas stream obtained by suitably mixing nitrogen gas with air for 2 hours to obtain a sintered body toroidal core having an outer diameter of 25 mm, an inner diameter of 15 mm, and a height of 5 mm, and five sintered cylindrical shapes having a diameter of 10 mm and a height of 10 mm. core.

再者,由於使用了高純度原料,故鐵氧體中含有的雜質P、B、S及Cl量均為5massppm。另外,P、B、S及Cl的含量是依據JIS K 0102(離子對層析法(Ion pair chromatography,IPC)質量分析法)進行定量。 Further, since a high-purity raw material was used, the amounts of impurities P, B, S, and Cl contained in the ferrite were all 5 mass ppm. Further, the contents of P, B, S and Cl were quantified in accordance with JIS K 0102 (Ion pair chromatography (IPC) mass spectrometry).

關於所獲得的試樣,基於JIS C 2560-2,於23℃下藉由阿基米德法對環形磁心測定燒結密度,並藉由四端子法測定比電阻。於環形磁心上實施10圈繞線,並根據使用電感電容電阻測試儀(inductance capacitance and resistance meter,LCR meter)(是德(Keysight)公司製造的4980A)所測定的電感來算出環形磁心的初透磁率。另外,居里溫度是根據電感的溫度特性測定結果而算出。關於磨耗值,依據日本粉末冶金協會(Japan Powder Metallurgy Association,JPMA)P11-1992中規定的方法進行測定。方形比是藉由將基於JIS C 2560-2並於23℃下測定的殘留磁通量密度Br除以飽和磁通量密度Bs而算出。 With respect to the obtained sample, the sintered density was measured for the toroidal core by the Archimedes method at 23 ° C based on JIS C 2560-2, and the specific resistance was measured by a four-terminal method. 10 turns of the winding on the toroidal core, and the initial measurement of the toroidal core is calculated according to the inductance measured by the inductance capacitance and resistance meter (LCR meter) (4980A manufactured by Keysight). Magnetic rate. Further, the Curie temperature is calculated based on the measurement result of the temperature characteristics of the inductor. The abrasion value was measured in accordance with the method specified in Japan Powder Metallurgy Association (JPMA) P11-1992. The square ratio was calculated by dividing the residual magnetic flux density Br measured at 23 ° C based on JIS C 2560-2 by the saturation magnetic flux density Bs.

將所獲得的結果一併記載於表1。 The obtained results are collectively shown in Table 1.

如表1所示般,於作為發明例的實施例1-1~實施例1-7中,可獲得兼具磨耗值未滿0.85%的高強度、以及23℃下的比電阻為30Ω.m以上、方形比為0.35以下且居里溫度100℃以上的優異磁特性的MnCoZn鐵氧體。 As shown in Table 1, in Examples 1-1 to 1-7 which are examples of the invention, a high strength having an abrasion value of less than 0.85% and a specific resistance at 23 ° C of 30 Ω were obtained. MnCoZn ferrite having excellent magnetic properties of m or more and a square ratio of 0.35 or less and a Curie temperature of 100 ° C or more.

相對於此,於含有50.0mol%以上的Fe2O3的比較例1-1、比較例1-2中,伴隨Fe2+的生成而比電阻大幅度下降。另一方面,於Fe2O3量未滿45.0mol%的比較例1-3中,觀察到方形比的上升及居里溫度的降低。 On the other hand, in Comparative Example 1-1 and Comparative Example 1-2 containing 50.0 mol% or more of Fe 2 O 3 , the specific resistance was greatly lowered with the formation of Fe 2+ . On the other hand, in Comparative Example 1-3 in which the amount of Fe 2 O 3 was less than 45.0 mol%, an increase in the square ratio and a decrease in the Curie temperature were observed.

另外,於ZnO量超出合理範圍的比較例1-4中,觀察到居里溫度的降低。另一方面,於ZnO量不滿足合理範圍的比較例1-5中,方形比上升,並且未能實現較佳的磁特性。 Further, in Comparative Example 1-4 in which the amount of ZnO exceeded the reasonable range, a decrease in the Curie temperature was observed. On the other hand, in Comparative Examples 1-5 in which the amount of ZnO did not satisfy a reasonable range, the square ratio was increased, and preferable magnetic characteristics were not achieved.

進而,於CoO量不滿足合理範圍的比較例1-6中,殘留磁通量密度提高,故方形比高,另一方面,於CoO量超出合理範圍的比較例1-7中,由於磁各向異性的提高而方形比亦變高,並且脫離較佳範圍。 Further, in Comparative Example 1-6 in which the amount of CoO did not satisfy a reasonable range, the residual magnetic flux density was increased, so the square ratio was high, and on the other hand, in Comparative Example 1-7 in which the amount of CoO exceeded the reasonable range, magnetic anisotropy was The increase and the square ratio also become higher and out of the preferred range.

實施例2 Example 2

於將所包含的鐵、鋅、鈷及錳全部換算為Fe2O3、ZnO、CoO及MnO的情況下,以Fe2O3量成為49.0mol%、ZnO量成為21.0mol%、CoO量成為2.0mol%及剩餘部分成為MnO組成的方式秤量原料,並使用球磨機混合16小時後,於空氣中以925℃進行3小時預煅燒。繼而,向該預煅燒粉中添加表2所示量的SiO2、CaO,利用球磨機進行12小時粉碎。繼而,向所獲得的粉碎漿料中添加 聚乙烯醇,於排風溫度250℃下進行噴霧乾燥造粒,通過孔徑350μm的篩而將粗粉去除後,施加118MPa的壓力而成形為環形磁心及圓柱磁心。再者,用於成形的造粒粉的粒度分佈d90為230μm,且壓碎強度為1.29MPa,鐵氧體中的雜質P、B、S及Cl量均為5massppm。 When all of the iron, zinc, cobalt, and manganese contained are converted into Fe 2 O 3 , ZnO, CoO, and MnO, the amount of Fe 2 O 3 is 49.0 mol%, the amount of ZnO is 21.0 mol%, and the amount of CoO becomes The raw material was weighed in a manner of 2.0 mol% and the remainder was made into a MnO composition, and after mixing for 16 hours using a ball mill, it was pre-calcined in air at 925 ° C for 3 hours. Then, SiO 2 and CaO in the amounts shown in Table 2 were added to the pre-calcined powder, and pulverization was carried out for 12 hours by a ball mill. Then, polyvinyl alcohol was added to the obtained pulverized slurry, spray-dried and granulated at an exhaust air temperature of 250 ° C, and the coarse powder was removed by a sieve having a pore size of 350 μm, and then a pressure of 118 MPa was applied to form a toroidal core and Cylindrical core. Further, the granulated powder for forming had a particle size distribution d90 of 230 μm and a crush strength of 1.29 MPa, and the amounts of impurities P, B, S and Cl in the ferrite were both 5 mass ppm.

其後,將該成形體放入煅燒爐中,於最高溫度1350℃下,於將氮氣與空氣適宜混合而成的氣流中煅燒2小時,獲得外徑:25mm、內徑:15mm、高度:5mm的燒結體環形磁心、與5個直徑:10mm、高度:10mm的圓柱形狀磁心。 Thereafter, the formed body was placed in a calcining furnace, and calcined in a gas stream obtained by suitably mixing nitrogen gas and air at a maximum temperature of 1,350 ° C for 2 hours to obtain an outer diameter of 25 mm, an inner diameter of 15 mm, and a height of 5 mm. The sintered body toroidal core, and five cylindrical cores having a diameter of 10 mm and a height of 10 mm.

對於所述各試樣,使用與實施例1相同的方法、裝置來評價各自的特性。 Each of the samples was evaluated for the respective characteristics by the same method and apparatus as in Example 1.

將所獲得的結果一併記載於表2。 The obtained results are collectively shown in Table 2.

如表2所示般,於SiO2量及CaO量為合理範圍內的實施例2-1~實施例2-4中,可獲得兼具磨耗值未滿0.85%的高強度、以及23℃下的比電阻為30Ω.m以上、方形比為0.35以下且居里溫度100℃以上的優異磁特性的MnCoZn鐵氧體。 As shown in Table 2, in Examples 2-1 to 2-4 in which the amount of SiO 2 and the amount of CaO were within a reasonable range, high strength at a wear value of less than 0.85% and a high strength at 23 ° C were obtained. The specific resistance is 30Ω. MnCoZn ferrite having excellent magnetic properties of m or more and a square ratio of 0.35 or less and a Curie temperature of 100 ° C or more.

相對於此,於SiO2、CaO中的任一者不滿足合理範圍的比較例2-1、比較例2-3中,晶界的生成不充分,因此晶粒的大小不整齊,故磨耗值高於0.85%,並且粒界厚度亦不充分,因此比電阻止於未滿30Ω.m。 On the other hand, in Comparative Example 2-1 and Comparative Example 2-3 in which either of SiO 2 and CaO did not satisfy a reasonable range, the generation of grain boundaries was insufficient, and thus the crystal grain size was not uniform, so the abrasion value was Above 0.85%, and the grain boundary thickness is not sufficient, so the specific electricity is prevented from less than 30Ω. m.

另外,於SiO2、CaO中的一者過多的比較例2-2、比較例2-4及比較例2-5水準,出現異常粒子,燒結受到阻礙,因此燒結密度低,且磨耗值亦高。此外,由於晶界的生成不充分,故比電阻低,且伴隨殘留磁通量密度的上升而方形比亦變高。 Further, in Comparative Example 2-2, Comparative Example 2-4, and Comparative Example 2-5 in which one of SiO 2 and CaO was excessive, abnormal particles appeared, and sintering was inhibited, so that the sintered density was low and the abrasion value was high. . Further, since the generation of the grain boundary is insufficient, the specific resistance is low, and the square ratio is also increased as the residual magnetic flux density increases.

實施例3 Example 3

藉由實施例1、實施例2所示的方法,使用如下原料來製作外徑:25mm、內徑:15mm、高度:5mm的燒結體環形磁心、與5個直徑:10mm、高度:10mm的圓柱形狀磁心,其中,所述原料中,成為使基本成分及副成分與實施例1-2為相同組成般的比例,另一方面,所含有的雜質量各不相同,使用與實施例1相同的方法、裝置來評價特性,將所獲得的結果示於表3。再者,用於成形的造粒粉的粒度分佈d90為230μm,並且壓碎強度為1.29MPa。 By the method shown in Example 1 and Example 2, a sintered body toroidal core having an outer diameter of 25 mm, an inner diameter of 15 mm, and a height of 5 mm was produced using the following materials, and five cylinders having a diameter of 10 mm and a height of 10 mm were used. In the shape of the raw material, the ratio of the basic component and the subcomponent to the same composition as in Example 1-2 is the same, and the amount of impurities contained in the raw material is different, and the same as in the first embodiment is used. The method and apparatus were used to evaluate the characteristics, and the results obtained are shown in Table 3. Further, the granulated powder for forming had a particle size distribution d90 of 230 μm and a crush strength of 1.29 MPa.

如表3所示般,於P、B、S及Cl的含量為規定值以下的實施例3-1中,獲得了由磨耗值表示的強度、以及由方形比、比電阻、及居里溫度表示的磁特性全部良好的值。 As shown in Table 3, in Example 3-1 in which the contents of P, B, S, and Cl were not more than the predetermined value, the strength expressed by the abrasion value, and the square ratio, the specific resistance, and the Curie temperature were obtained. The magnetic properties indicated are all good values.

相對於此,該四個水準中的一個或多個超過了規定值的比較例3-1~比較例3-6均出現了異常粒子,且燒結受到阻礙,因此燒結密度低,故磨耗值高,而且晶界的生成不充分,故比電阻低,進而伴隨殘留磁通量密度的上升而方形比亦變高。 On the other hand, in Comparative Example 3-1 to Comparative Example 3-6 in which one or more of the four levels exceeded a predetermined value, abnormal particles appeared, and sintering was hindered, so that the sintered density was low, so the abrasion value was high. Further, since the formation of the grain boundary is insufficient, the specific resistance is low, and the square ratio is also increased as the residual magnetic flux density increases.

實施例4 Example 4

於表4所示的各種溫度條件下,對藉由實施例1、實施例2所示的方法、且以基本成分、副成分及雜質成分成為與實施例1-2相同的組成般的比例所製作的成形體進行煅燒。 Under the various temperature conditions shown in Table 4, the ratios of the basic composition, the subcomponent, and the impurity component in the same manner as in Example 1-2 were obtained by the methods shown in Example 1 and Example 2. The produced shaped body was calcined.

對於所述各試樣,使用與實施例1相同的方法、裝置來評價各自的特性。將所獲得的結果一併記載於表4。再者,用於成形的造粒粉的粒度分佈d90為230μm,並且壓碎強度為1.29MPa。 Each of the samples was evaluated for the respective characteristics by the same method and apparatus as in Example 1. The obtained results are collectively shown in Table 4. Further, the granulated powder for forming had a particle size distribution d90 of 230 μm and a crush strength of 1.29 MPa.

如表4所示般,於以煅燒時的最高保持溫度為1290℃以上、且保持時間為1小時以上進行煅燒、燒結密度為4.85g/cm3以上的實施例3-1~實施例3-5中,由磨耗值表示的強度、以及由比電阻、方形比及居里溫度表示的磁特性均良好。 As shown in Table 4, Example 3-1 to Example 3 were carried out in which the maximum holding temperature at the time of firing was 1290 ° C or higher and the holding time was 1 hour or longer, and the sintered density was 4.85 g/cm 3 or more. In 5, the strength represented by the abrasion value and the magnetic characteristics represented by the specific resistance, the square ratio, and the Curie temperature were good.

相對於此,於煅燒溫度未滿1290℃、或者保持時間未滿1小時、燒結密度未滿4.85g/cm3的比較例3-1~比較例3-6中,由於燒結密度低,故磨耗值變高,且晶粒生長不充分,故磁滯損失增大,且殘留磁通量密度Br上升,結果,方形比變高,就強度、磁特性兩者的觀點而言欠佳。 On the other hand, in Comparative Example 3-1 to Comparative Example 3-6 in which the calcination temperature was less than 1290 ° C or the holding time was less than 1 hour and the sintered density was less than 4.85 g/cm 3 , since the sintered density was low, the abrasion was performed. When the value is high and the crystal grain growth is insufficient, the hysteresis loss increases and the residual magnetic flux density Br increases. As a result, the square ratio becomes high, which is not preferable from the viewpoint of both strength and magnetic properties.

實施例5 Example 5

使用藉由實施例1、實施例2所示的方法,且以與實施例1-2相同的組成、相同的噴霧乾燥條件所獲得的造粒粉,並變更過篩條件,藉此成為表5所示的粒度分佈d90的值,對成為所述值的造粒粉(壓碎強度:1.29MPa)施加118MPa的壓力而成形為環形磁心及圓柱磁心。其後,將該成形體放入煅燒爐中,於最高溫度1350℃下,於將氮氣與空氣適宜混合而成的氣流中煅燒2小時,獲得外徑:25mm、內徑:15mm、高度:5mm的燒結體環形磁心、與5個直徑:10mm、高度:10mm的圓柱形狀磁心。 Using the method shown in Example 1 and Example 2, and the granulated powder obtained by the same composition and the same spray drying conditions as in Example 1-2, and changing the sieving conditions, Table 5 was used. The value of the particle size distribution d90 shown was applied to the granulated powder (crushing strength: 1.29 MPa) having the above value to form a toroidal core and a cylindrical core. Thereafter, the formed body was placed in a calcining furnace, and calcined in a gas stream obtained by suitably mixing nitrogen gas and air at a maximum temperature of 1,350 ° C for 2 hours to obtain an outer diameter of 25 mm, an inner diameter of 15 mm, and a height of 5 mm. The sintered body toroidal core, and five cylindrical cores having a diameter of 10 mm and a height of 10 mm.

對於所述各試樣,使用與實施例1相同的方法、裝置來評價各自的特性。將所獲得的結果一併記載於表5。 Each of the samples was evaluated for the respective characteristics by the same method and apparatus as in Example 1. The obtained results are collectively shown in Table 5.

如表5所示般,於造粒粉粒度分佈d90的值為300μm以下的實施例5-1中,造粒粉間的空隙的殘存少,缺損的起點少,故可將磨耗值抑制為0.85%以下。 As shown in Table 5, in Example 5-1 in which the particle size distribution d90 of the granulated powder was 300 μm or less, the amount of voids between the granulated powders was small, and the starting point of the defects was small, so that the abrasion value was suppressed to 0.85. %the following.

相對於此,於d90的值大於300μm的比較例5-1~比較例5-3中,造粒粉間的空隙多,缺損的起點多,因此磨耗值高,強度降低。 On the other hand, in Comparative Example 5-1 to Comparative Example 5-3 in which the value of d90 was more than 300 μm, since there were many voids between the granulated powder and many starting points of the defect, the abrasion value was high and the strength was lowered.

實施例6 Example 6

於表6所示的排風溫度條件下對藉由實施例1、實施例2所示的方法製作的、以與實施例1-2相同的組成製作的漿料進行噴霧乾燥,藉此獲得壓碎強度不同的造粒粉,使其通過孔徑350μm的篩而將粗粉去除後,施加118MPa的壓力而成形為環形磁心及圓柱磁心。再者,此時的造粒粉的粒度分佈d90為230μm。 The slurry prepared by the method shown in Example 1 and Example 2, which was produced by the method shown in Example 1 and Example 2, was spray-dried under the exhaust air temperature conditions shown in Table 6, thereby obtaining a pressure. The granulated powder having different crushing strengths was passed through a sieve having a pore size of 350 μm to remove the coarse powder, and then a pressure of 118 MPa was applied to form a toroidal core and a cylindrical core. Further, the particle size distribution d90 of the granulated powder at this time was 230 μm.

其後,將該成形體放入煅燒爐中,於最高溫度1350℃下,於將氮氣與空氣適宜混合而成的氣流中煅燒2小時,獲得外徑:25mm、內徑:15mm、高度:5mm的燒結體環形磁心、與5個直徑:10mm、高度:10mm的圓柱形狀磁心。 Thereafter, the formed body was placed in a calcining furnace, and calcined in a gas stream obtained by suitably mixing nitrogen gas and air at a maximum temperature of 1,350 ° C for 2 hours to obtain an outer diameter of 25 mm, an inner diameter of 15 mm, and a height of 5 mm. The sintered body toroidal core, and five cylindrical cores having a diameter of 10 mm and a height of 10 mm.

對於所述各試樣,使用與實施例1相同的方法、裝置來評價各自的特性。將所獲得的結果一併記載於表6。 Each of the samples was evaluated for the respective characteristics by the same method and apparatus as in Example 1. The obtained results are collectively shown in Table 6.

如表6所示般,於噴霧乾燥造粒的排風溫度不過高的實施例6-1中,造粒粉的壓碎強度未滿1.5MPa,於成形時造粒粉充分破壞,因此未殘留造粒粉間的間隙,因此,缺損的起點少,故可將磨耗值抑制為未滿0.85%。 As shown in Table 6, in Example 6-1 in which the exhaust air temperature of the spray-drying granulation was not excessively high, the crushing strength of the granulated powder was less than 1.5 MPa, and the granulated powder was sufficiently destroyed at the time of molding, so that no residue remained. Since the gap between the granulated powders is small, the starting point of the defects is small, so that the abrasion value can be suppressed to less than 0.85%.

相對於此,若著眼於排風溫度過高、造粒粉壓碎強度為1.5MPa以上的比較例6-1~比較例6-3,則由造粒粉破壞不良所引起的缺損的起點多,因此磨耗值變高,強度降低。 On the other hand, in the case of Comparative Example 6-1 to Comparative Example 6-3 in which the exhaust gas temperature is too high and the granulated powder crushing strength is 1.5 MPa or more, the starting point of the defect caused by the granulated powder destruction failure is large. Therefore, the wear value becomes high and the strength is lowered.

Claims (7)

一種MnCoZn系鐵氧體,其中,作為基本成分,包含鐵:以Fe2O3換算計為47.1mol%以上且未滿50.0mol%、鋅:以ZnO換算計為15.5mol%~24.0mol%、鈷:以CoO換算計為0.5mol%~4.0mol%及錳:作為剩餘部分,以MnO換算計為26.5mol%~32.0mol%,相對於所述基本成分而言,作為副成分,包含SiO2:50massppm~300massppm及CaO:300massppm~1300massppm,且剩餘部分包含不可避免的雜質,將所述不可避免的雜質中的P、B、S及Cl量分別抑制為P:未滿50massppm、B:未滿20massppm、S:未滿30massppm及Cl:未滿50massppm,進而,於所述MnCoZn系鐵氧體中,磨耗值未滿0.85%,23℃下的方形比為0.35以下,比電阻為30Ω.m以上,以及居里溫度為100℃以上。 A MnCoZn-based ferrite containing, as a basic component, iron: 47.1 mol% or more and less than 50.0 mol% in terms of Fe 2 O 3 and zinc: 15.5 mol% to 24.0 mol% in terms of ZnO. Cobalt: 0.5 mol% to 4.0 mol% in terms of CoO and manganese: 26.5 mol% to 32.0 mol% in terms of MnO as a remainder, and SiO 2 as a subcomponent as a subcomponent : 50 mass ppm to 300 mass ppm and CaO: 300 mass ppm to 1300 mass ppm, and the remainder contains unavoidable impurities, and the amounts of P, B, S, and Cl in the unavoidable impurities are respectively suppressed to P: less than 50 mass ppm, B: not full 20 mass ppm, S: less than 30 mass ppm, and Cl: less than 50 mass ppm. Further, in the MnCoZn ferrite, the abrasion value is less than 0.85%, the square ratio at 23 ° C is 0.35 or less, and the specific resistance is 30 Ω. m or more, and the Curie temperature is 100 ° C or more. 如申請專利範圍第1項所述的MnCoZn系鐵氧體,其 中,所述MnCoZn系鐵氧體的燒結密度為4.85g/cm3以上。 The MnCoZn-based ferrite according to the first aspect of the invention, wherein the MnCoZn-based ferrite has a sintered density of 4.85 g/cm 3 or more. 如申請專利範圍第1項或第2項所述的MnCoZn系鐵氧體,其中,所述MnCoZn系鐵氧體為包含粒度分佈d90的值為300μm以下的造粒粉的成形-燒結體的MnCoZn系鐵氧體。 The MnCoZn-based ferrite according to the first or second aspect of the invention, wherein the MnCoZn-based ferrite is a shaped-sintered MnCoZn of a granulated powder having a particle size distribution d90 of 300 μm or less. Ferrite. 如申請專利範圍第1項或第2項所述的MnCoZn系鐵氧體,其中,所述MnCoZn系鐵氧體為包含壓碎強度未滿1.50MPa的造粒粉的成形-燒結體的MnCoZn系鐵氧體。 The MnCoZn-based ferrite according to the first or second aspect of the invention, wherein the MnCoZn-based ferrite is a MnCoZn system of a formed-sintered body comprising a granulated powder having a crushing strength of less than 1.50 MPa. Ferrite. 如申請專利範圍第3項所述的MnCoZn系鐵氧體,其中,所述MnCoZn系鐵氧體為包含壓碎強度未滿1.50MPa的造粒粉的成形-燒結體的MnCoZn系鐵氧體。 The MnCoZn-based ferrite according to the third aspect of the invention, wherein the MnCoZn-based ferrite is a molded-sintered MnCoZn-based ferrite containing a granulated powder having a crush strength of less than 1.50 MPa. 一種MnCoZn系鐵氧體的製造方法,其包括:預煅燒步驟,對以成為規定的成分比率的方式秤量的基本成分的混合物進行預煅燒;混合-粉碎步驟,向所述預煅燒步驟中所得的預煅燒粉中添加已調整為規定比率的副成分,並加以混合、粉碎;以及煅燒步驟,向所述混合-粉碎步驟中所得的粉碎粉中添加黏合劑並加以混合後,以造粒粉的粒度分佈d90的值成為300μm以下及/或壓碎強度未滿1.50MPa的方式進行造粒,並將所得的所述造粒粉加以成形後,於最高保持溫度:1290℃以上、保持時間:1小時以上的條件下進行煅燒,從而獲得如申請專利範圍第1項或第2項所述的MnCoZn系鐵氧體。 A method for producing a MnCoZn-based ferrite, comprising: a pre-calcining step of pre-calcining a mixture of basic components weighed so as to have a predetermined component ratio; and a mixing-pulverizing step, which is obtained in the pre-calcining step a pre-calcined powder is added with a sub-component adjusted to a predetermined ratio, and mixed and pulverized; and a calcination step, a binder is added to the pulverized powder obtained in the mixing-pulverizing step, and mixed, and then granulated powder is used. The granulation is carried out so that the value of the particle size distribution d90 is 300 μm or less and/or the crush strength is less than 1.50 MPa, and the obtained granulated powder is molded, and the maximum holding temperature is 1290 ° C or higher, and the holding time is 1 The calcination is carried out under the conditions of an hour or more to obtain the MnCoZn-based ferrite as described in the first or second aspect of the patent application. 如申請專利範圍第6項所述的MnCoZn系鐵氧體的製 造方法,其中,所述造粒為噴霧乾燥法。 Manufacture of MnCoZn ferrite as described in claim 6 The method of producing, wherein the granulation is a spray drying method.
TW107120211A 2017-08-29 2018-06-12 MnCoZn ferrite and manufacturing method thereof TWI667220B (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
JP2017-164698 2017-08-29
JP2017164698 2017-08-29

Publications (2)

Publication Number Publication Date
TW201912609A TW201912609A (en) 2019-04-01
TWI667220B true TWI667220B (en) 2019-08-01

Family

ID=65525771

Family Applications (1)

Application Number Title Priority Date Filing Date
TW107120211A TWI667220B (en) 2017-08-29 2018-06-12 MnCoZn ferrite and manufacturing method thereof

Country Status (3)

Country Link
CN (1) CN110325489B (en)
TW (1) TWI667220B (en)
WO (1) WO2019044060A1 (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP6732159B1 (en) * 2019-03-18 2020-07-29 Jfeケミカル株式会社 MnCoZn ferrite and method for producing the same
WO2020189035A1 (en) * 2019-03-18 2020-09-24 Jfeケミカル株式会社 MnCoZn FERRITE AND METHOD FOR PRODUCING SAME
CN111233452B (en) * 2019-10-18 2021-09-17 横店集团东磁股份有限公司 High-frequency high-impedance lean iron manganese zinc ferrite and preparation method thereof
WO2022014219A1 (en) * 2020-07-14 2022-01-20 Jfeケミカル株式会社 Mncozn-based ferrite

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN105418059A (en) * 2014-09-17 2016-03-23 Tdk株式会社 Ferrite composite for wave absorber and wave absorber

Family Cites Families (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0462908A (en) * 1990-07-02 1992-02-27 Tokin Corp Manufacture of low loss oxide magnetic material
JP4694973B2 (en) * 2006-01-26 2011-06-08 Jfeフェライト株式会社 MnCoZn ferrite and transformer core
JP2008184363A (en) * 2007-01-30 2008-08-14 Fdk Corp MnZn-BASED FERRITE AND METHOD FOR PRODUCING THE SAME
JP4488051B2 (en) * 2007-10-19 2010-06-23 Tdk株式会社 Radio wave absorber
JP5546139B2 (en) * 2009-01-29 2014-07-09 Jfeケミカル株式会社 MnZnCo ferrite core and method for producing the same
JP2010180101A (en) * 2009-02-06 2010-08-19 Jfe Chemical Corp HIGH RESISTANCE AND HIGHLY SATURATED MAGNETIC FLUX DENSITY MnZnCo FERRITE, AND METHOD FOR PRODUCING THE SAME
JP2017075085A (en) * 2015-10-16 2017-04-20 Tdk株式会社 MnZnLi-BASED FERRITE, MAGNETIC CORE AND TRANSFORMER

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN105418059A (en) * 2014-09-17 2016-03-23 Tdk株式会社 Ferrite composite for wave absorber and wave absorber

Also Published As

Publication number Publication date
TW201912609A (en) 2019-04-01
WO2019044060A1 (en) 2019-03-07
CN110325489B (en) 2021-11-12
CN110325489A (en) 2019-10-11

Similar Documents

Publication Publication Date Title
TWI667220B (en) MnCoZn ferrite and manufacturing method thereof
TWI667200B (en) MnCoZn series ferrite and manufacturing method thereof
JP6462959B1 (en) Rod-shaped MnZn ferrite core, manufacturing method thereof, and antenna
JP2005213100A (en) METHOD OF MANUFACTURING MnZn FERRITE AND MnZn FERRITE
JP2004217452A (en) Ferrite material and method of manufacturing the same
KR20080037521A (en) Hexagonal z type ferrite sintered material and method of fabricating the same
JP2023075218A (en) MnZn BASED FERRITE POWDER
JP7182016B2 (en) MnCoZn ferrite
CN110418775B (en) MnCoZn ferrite and method for producing same
TWI692462B (en) MnCoZn series ferrite iron and its manufacturing method
TWI694059B (en) MnCoZn series ferrite iron and its manufacturing method
TWI704122B (en) Manganese-cobalt-zinc fertilizer granular iron and its manufacturing method
WO2022070634A1 (en) MnZn-BASED FERRITE AND METHOD OF MANUFACTURING SAME
JP6439086B1 (en) MnCoZn-based ferrite and method for producing the same
CN110418776B (en) MnCoZn ferrite and method for producing same
JPWO2020158334A1 (en) MnCoZn-based ferrite and its manufacturing method
TWI727622B (en) Manganese-zinc fertilizer granulated iron and its manufacturing method
CN114206805B (en) MnZn ferrite
JP5952236B2 (en) Mn-Zn-Ni ferrite and method for producing the same
JP2005170763A (en) Mn/Zn FERRITE, ITS MANUFACTURING METHOD AND ELECTRONIC PART
JP2004238211A (en) Manganese-zinc ferrite