JPH0353270B2 - - Google Patents
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- JPH0353270B2 JPH0353270B2 JP56113311A JP11331181A JPH0353270B2 JP H0353270 B2 JPH0353270 B2 JP H0353270B2 JP 56113311 A JP56113311 A JP 56113311A JP 11331181 A JP11331181 A JP 11331181A JP H0353270 B2 JPH0353270 B2 JP H0353270B2
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- manganese
- magnetic
- niobium oxide
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Description
本発明は、低損失、低残留磁束密度の新規マン
ガン−亜鉛系フエライト磁性材料の製造方法に関
するものである。
マンガン−亜鉛系フエライトは、各種通信機
器、民生用機器などのトランス材料として多用さ
れているが、最近に至り電源を小型化するため周
波数の高い電源が使用される傾向があり、その目
的に適うトランス材料としての性質が要求される
ようになつてきた。
この高周波電源用としてのマンガン−亜鉛系フ
エライトに要求される性質には、高密度、高抵抗
性、高透磁率、高飽和磁束密度、低残留磁束密度
及びトランスの作動温度近傍における低電力損失
などがある。
これまで、マンガン−亜鉛系フエライトの電磁
気特性を改善するには、種々の微量成分を添加す
ることが行われ、CaCO3−SiO2複合添加(特公
昭36−2283号公報)や、SnO2−TiO2複合添加
(特公昭51−48276号公報)によつて、磁芯特性が
改善されることが知られている。
しかしながら、これらのマンガン−亜鉛系フエ
ライトは、渦電流損失などの点でかなりの特性向
上は認められるが、高温における電力損失の点で
まだ十分満足できるものとはいえない。
本発明者らは、高周波電源用トランス材料に適
したマンガン−亜鉛系フエライトを開発するため
に、鋭意研究を重ねた結果、微量成分として酸化
ニオブを添加し、適正な製造プロセスにより加熱
焼結した場合、非常に優れた電磁気特性が得られ
ることを見出し、この知見に基づいて本発明をな
すに至つた。
これまで、マンガン−亜鉛系フエライトに酸化
ニオブを添加して高透磁率、低損失のものとする
ことは知られている(特公昭38−23421号公報)。
しかしながら、このようにして得られたフエライ
トは、低周波数領域、常温領域においては、高い
透磁率や低い渦電流損失を示すが、高周波電源用
としての、100KHz、100℃以上という苛酷な条件
下では、上記の特性は著しく低下し、実用に供す
ることができない。本発明は、製造プロセスに工
夫を加えることにより、これらの難点を克服し、
全く新らしい特性を有する磁性材料を提供したも
のである。
すなわち、本発明は、マンガン−亜鉛系フエラ
イトを製造するに当り、原料混合物中に微量成分
として酸化ニオブ又は焼成により酸化ニオブを生
じる化合物Nb2O5換算で0.02〜0.10重量%の割合
で添加したのち、大気圧下における徐熱工程及び
酸素濃度を制御した雰囲気下における急熱工程を
経て所定の燃結温度まで昇温させ、この温度にお
いて燃結を完了させることを特徴とする、B−H
ループのBm/Brが3.0以上であつて、かつ100K
Hz、2000G、100℃の条件下での電力損失が450m
W/c.c.以下である磁性材料の製造方法を提供する
ものである。
本発明方法において添加する酸化ニオブは、低
温高密度焼結を可能とし、磁芯特性を効果的に改
善するために含有させるものであるが、これは原
料の全量当り0.02〜0.10重量%の範囲内で含有さ
せることが必要である。この量が0.02重量%未満
では、製造条件をどのように制御しても磁芯特性
の改善がなされないし、またこの量が0.10重量%
を超えると、焼結過程の制御が困難になり結果的
に磁芯特性の劣化をもたらす。
本発明方法により得られる磁性材料において
は、酸化鉄、酸化マンガン、酸化亜鉛及び酸化ニ
オブ以外の成分を特に含有させる必要はないが、
原料に起因する不純分、製造過程中に混入する汚
染物質、あるいは酸化ニオブの効果を阻害しない
程度の他の微量成分例えばCaCO3、SiO2、
Ta2O5、TiO2などの添加は許容される。
本発明方法においては、磁性材料を、制御され
た特定の製造工程に従つて製造することが必要で
ある。すなわち、本発明方法に従えば、マンガン
−亜鉛系フエライトを製造するに当り、原料混合
物中に微量成分として酸化ニオブを生じる化合物
をNb2O5換算で0.02〜0.10重量%の割合で添加し
たのち、大気圧下における徐熱工程及び酸素濃度
を制御した雰囲気下における急熱工程を経て所定
の焼結温度まで昇温させ、その温度において焼結
を完了させることにより前記の磁性材料を得るこ
とができる。
本発明方法における主原料としては、酸化鉄成
分と酸化マンガン成分と酸化亜鉛成分の混合物が
用いられる。この酸化鉄成分としては、Fe2O3、
FeO、Fe3O4などの酸化物のほか、焼成により酸
化鉄に変ることのできる化合物、例えば水酸化
鉄、シユウ酸鉄などが用いられる。また、酸化マ
ンガン成分としては、MnO、MnO2、Mn3O4な
どの酸化物のほか、炭酸マンガン、シユウ酸マン
ガンなどの焼成により酸化マンガンに変わること
のできる化合物が用いられる。さらに酸化亜鉛と
しては、ZnOのような酸化物のほか、炭酸亜鉛、
シユウ酸亜鉛などの焼成により酸化亜鉛に変わる
ことのできる化合物が用いられる。
これらの酸化鉄成分、酸化マンガン成分及び酸
化亜鉛成分は、磁性材料の最終組成としてそれぞ
れFe2O3換算52〜54.5モル%、MnO換算25〜37モ
ル%、ZnO換算7〜21モル%の割合になるように
混合され、原料として供される。
地方、本発明の磁性材料中に含有させる酸化ニ
オブは、通常Nb2O5として原料混合物中に添加す
るが、例えば炭酸塩又はシユウ酸塩のように焼成
することにより最終製品中にNb2O5の形で含まれ
うるものを用いることもできる。
本発明方法により、所望の磁性材料を好適に製
造するには、先ず原料混合物を800〜1000℃の温
度で仮焼成し、仮焼品を粉砕し、これに適当なバ
インダー例えばポリビニルアルコールを少量加え
て成形する。次いで、この成形品を大気圧下、
800〜1100℃の範囲内の所定温度まで、200〜350
℃/hrの昇温速度で急熱後、その温度から1000〜
1150℃の範囲内のあらかじめ選択された温度ま
で、30〜70℃/hrの昇温速度で徐熱する。次いで
酸素濃度を制御した雰囲気下において、所要の焼
結温度まで200〜350℃/hrの昇温速度で急熱し、
その温度で焼結を完了させる。この際の焼成雰囲
気条件としては、酸素濃度を0.1〜5%程度に制
御した窒素雰囲気が好ましく焼成はこの中で通常
1250〜1350℃の範囲の所定温度に、1〜10時間保
持することによつて行われる。
このようにして焼結が完了した後の冷却工程
は、焼結温度から1100〜1200℃程度までは温度に
応じて酸素濃度を制御した雰囲気で、それ以降は
不活性雰囲気例えば窒素雰囲気下で行うのが好ま
しい。冷却速度としては、通常200〜350℃/hrの
範囲が用いられる。
このようにして得られる磁性材料は、B−Hル
ープのBm/Brが3.0以上、周波数100KHz、磁束
密度2000G、温度100℃の条件下での電力損失が
450mW/c.c.以下という特性によつて特徴づけら
れる。すなわち、この磁性材料は、飽和磁束密度
Bmが大きく、残留磁束密度Brが小さいため、
Bm−Brが大きくなると同時に、また高周波、高
磁束密度、高温領域における電力損失が少ないと
いう特徴を有している。
したがつて、この磁性材料は高周波電源用トラ
ンスの磁芯として好適である。
次に実施例によつて本発明をさらに詳細に説明
する。
実施例 1
Fe2O353.7モル%、ZnO10.6モル%及び
MnO35.7モル%から成る原料混合物に微量成分
として第1表に示す量のCaCO3とNb2O5を添加
し、常法に従つて950℃で仮焼成したのち、湿式
ボールミルで粉砕し、平均粒径1.0μの粉末とし
た。
次にこの仮焼物にバインダーとしてポリビニル
アルコールを加え、リング状に成形し、大気中に
おいて900℃まで加熱したのち、1050℃まで50
℃/hrの昇温速度で徐熱した。次いで0.5%の酸
素を含む雰囲気下において1320℃まで300℃/hr
の昇温速度で急熱し、この温度に3時間保持して
焼結を完了させたのち、炉の電源を切つて冷却を
開始し、1200℃に達したとき、純窒素雰囲気に切
替え、室温まで冷却した。
このようにして得られた6種の磁性材料の磁気
特性を第1表に示す。
The present invention relates to a method for producing a new manganese-zinc ferrite magnetic material with low loss and low residual magnetic flux density. Manganese-zinc ferrite is widely used as a transformer material in various communications equipment and consumer equipment, but recently there has been a trend toward using higher frequency power supplies to miniaturize power supplies, and it is suitable for this purpose. Properties as transformer materials have come to be required. The properties required of manganese-zinc ferrite for use in high-frequency power supplies include high density, high resistance, high magnetic permeability, high saturation magnetic flux density, low residual magnetic flux density, and low power loss near the operating temperature of the transformer. There is. Until now, various trace components have been added to improve the electromagnetic properties of manganese-zinc ferrite, such as combined addition of CaCO 3 -SiO 2 (Japanese Patent Publication No. 36-2283) and SnO 2 - It is known that the magnetic core properties are improved by TiO 2 composite addition (Japanese Patent Publication No. 51-48276). However, although these manganese-zinc ferrites show considerable improvement in characteristics in terms of eddy current loss, etc., they are still not fully satisfactory in terms of power loss at high temperatures. In order to develop manganese-zinc ferrite suitable for transformer materials for high-frequency power supplies, the inventors of the present invention have conducted intensive research and have added niobium oxide as a trace component and heated and sintered it using an appropriate manufacturing process. The inventors have discovered that very excellent electromagnetic properties can be obtained when using the same method, and based on this finding, the present invention has been accomplished. Hitherto, it has been known to add niobium oxide to manganese-zinc ferrite to make it have high magnetic permeability and low loss (Japanese Patent Publication No. 38-23421).
However, the ferrite obtained in this way shows high magnetic permeability and low eddy current loss in the low frequency region and room temperature region, but under the harsh conditions of 100KHz and 100℃ or more for high frequency power supply. , the above characteristics are significantly deteriorated and it cannot be put to practical use. The present invention overcomes these difficulties by adding innovation to the manufacturing process.
This provides a magnetic material with completely new properties. That is, in producing manganese-zinc ferrite, the present invention adds niobium oxide or a compound Nb 2 O 5 which produces niobium oxide as a trace component to the raw material mixture at a ratio of 0.02 to 0.10% by weight in terms of Nb 2 O 5. B-H is characterized in that it is then heated to a predetermined sintering temperature through a gradual heating step under atmospheric pressure and a rapid heating step in an atmosphere with controlled oxygen concentration, and combustion is completed at this temperature.
Bm/Br of the loop is 3.0 or more and 100K
Power loss is 450m under Hz, 2000G, 100℃ conditions
The present invention provides a method for manufacturing a magnetic material having a W/cc or less. Niobium oxide is added in the method of the present invention to enable low-temperature, high-density sintering and to effectively improve the magnetic core properties, but this is in the range of 0.02 to 0.10% by weight based on the total amount of raw materials. It is necessary to contain it within the range. If this amount is less than 0.02% by weight, the magnetic core characteristics will not be improved no matter how the manufacturing conditions are controlled, and if this amount is less than 0.10% by weight
If it exceeds this, it becomes difficult to control the sintering process, resulting in deterioration of the magnetic core properties. In the magnetic material obtained by the method of the present invention, it is not necessary to specifically contain components other than iron oxide, manganese oxide, zinc oxide, and niobium oxide;
Impurities caused by raw materials, contaminants mixed in during the manufacturing process, or other trace components that do not inhibit the effects of niobium oxide, such as CaCO 3 , SiO 2 ,
Additions such as Ta 2 O 5 and TiO 2 are allowed. The method of the invention requires that the magnetic material be manufactured according to a controlled and specific manufacturing process. That is, according to the method of the present invention, in producing manganese-zinc ferrite, after adding a compound that produces niobium oxide as a trace component to the raw material mixture at a ratio of 0.02 to 0.10% by weight calculated as Nb 2 O 5 . The above magnetic material can be obtained by raising the temperature to a predetermined sintering temperature through a gradual heating step under atmospheric pressure and a rapid heating step in an atmosphere with controlled oxygen concentration, and completing sintering at that temperature. can. As the main raw material in the method of the present invention, a mixture of an iron oxide component, a manganese oxide component, and a zinc oxide component is used. This iron oxide component includes Fe 2 O 3 ,
In addition to oxides such as FeO and Fe 3 O 4 , compounds that can be converted into iron oxide by firing, such as iron hydroxide and iron oxalate, are used. Further, as the manganese oxide component, in addition to oxides such as MnO, MnO 2 , and Mn 3 O 4 , compounds that can be converted into manganese oxide by firing, such as manganese carbonate and manganese oxalate, are used. Furthermore, as zinc oxide, in addition to oxides such as ZnO, zinc carbonate,
Compounds that can be converted to zinc oxide by calcination, such as zinc oxalate, are used. These iron oxide components, manganese oxide components, and zinc oxide components have a ratio of 52 to 54.5 mol% in terms of Fe 2 O 3 , 25 to 37 mol% in terms of MnO, and 7 to 21 mol% in terms of ZnO, respectively, as the final composition of the magnetic material. It is mixed so that it becomes the same and used as a raw material. Generally speaking, the niobium oxide contained in the magnetic material of the present invention is usually added as Nb 2 O 5 to the raw material mixture, but it can be converted into Nb 2 O in the final product by calcination, such as carbonate or oxalate. 5 can also be used. In order to suitably produce a desired magnetic material by the method of the present invention, first, the raw material mixture is calcined at a temperature of 800 to 1000°C, the calcined product is crushed, and a small amount of a suitable binder such as polyvinyl alcohol is added thereto. and mold it. Next, this molded product is placed under atmospheric pressure.
200-350 to a specified temperature within the range of 800-1100℃
After rapid heating at a heating rate of ℃/hr, the temperature rises to 1000~
Slow heat to a preselected temperature within the range of 1150°C at a heating rate of 30-70°C/hr. Next, in an atmosphere with controlled oxygen concentration, the material is rapidly heated to the required sintering temperature at a heating rate of 200 to 350°C/hr.
Sintering is completed at that temperature. The firing atmosphere conditions at this time are preferably a nitrogen atmosphere with an oxygen concentration controlled to about 0.1 to 5%.
This is carried out by maintaining a predetermined temperature in the range of 1250 to 1350°C for 1 to 10 hours. The cooling process after sintering is completed in this way is carried out in an atmosphere where the oxygen concentration is controlled according to the temperature from the sintering temperature to about 1100-1200℃, and thereafter in an inert atmosphere, such as a nitrogen atmosphere. is preferable. The cooling rate is usually in the range of 200 to 350°C/hr. The magnetic material obtained in this way has a B-H loop Bm/Br of 3.0 or more, a frequency of 100 KHz, a magnetic flux density of 2000 G, and a power loss of 100°C.
It is characterized by a property of 450mW/cc or less. In other words, this magnetic material has a saturation magnetic flux density
Since Bm is large and residual magnetic flux density Br is small,
At the same time as Bm-Br becomes large, it also has the characteristics of low power loss in high frequency, high magnetic flux density, and high temperature regions. Therefore, this magnetic material is suitable as a magnetic core of a transformer for high frequency power supply. Next, the present invention will be explained in more detail with reference to Examples. Example 1 Fe 2 O 3 53.7 mol%, ZnO 10.6 mol% and
CaCO 3 and Nb 2 O 5 in amounts shown in Table 1 were added as trace components to a raw material mixture consisting of 5.7 mol % of MnO3, calcined at 950°C according to a conventional method, and then ground in a wet ball mill. It was made into a powder with an average particle size of 1.0μ. Next, polyvinyl alcohol is added as a binder to this calcined product, formed into a ring shape, heated to 900℃ in the atmosphere, and then heated to 1050℃ for 50 minutes.
The temperature was gradually increased at a temperature increase rate of °C/hr. Then 300℃/hr up to 1320℃ in an atmosphere containing 0.5% oxygen
After heating up rapidly at a temperature increase rate of 3 hours and completing sintering by holding at this temperature for 3 hours, the furnace was turned off and cooling started. When the temperature reached 1200℃, the atmosphere was switched to pure nitrogen and the temperature was lowered to room temperature. Cooled. Table 1 shows the magnetic properties of the six types of magnetic materials thus obtained.
【表】
この表から分るように、CaCO3の添加は残留
磁束密度(Br)の低下に対し有効であるが、同
時に飽和磁束密度(Bm)も低下させ、したがつ
てBm/Brの増大は得られない。他方、Nb2O5の
添加はBmを増大するとともにBrを減少させるの
でBm/Brは著しく増大させる。
また、高周波、高磁束密度、高温領域下におけ
る電力損失は、Nb2O5の添加、特に0.05重量%程
度の添加により著しく低くなつている。
実施例 2
実施例1と同じ組成のマンガン−亜鉛系フエラ
イトに、微量成分としてCaCO3、Nb2O5及び
V2O5を含有させ、磁芯特性を測定した。この際
の磁性材料の製造条件としては、実施例1と同じ
条件を用いた。得られた結果を第2表に示す。[Table] As can be seen from this table, the addition of CaCO 3 is effective in reducing the residual magnetic flux density (Br), but it also reduces the saturation magnetic flux density (Bm) and therefore increases Bm/Br. cannot be obtained. On the other hand, addition of Nb 2 O 5 increases Bm and decreases Br, so Bm/Br increases significantly. Furthermore, the power loss under high frequency, high magnetic flux density, and high temperature ranges is significantly lowered by the addition of Nb 2 O 5 , particularly by the addition of about 0.05% by weight. Example 2 CaCO 3 , Nb 2 O 5 and trace components were added to manganese-zinc ferrite having the same composition as in Example 1.
V 2 O 5 was added and the magnetic core properties were measured. The same conditions as in Example 1 were used as the manufacturing conditions for the magnetic material at this time. The results obtained are shown in Table 2.
【表】
マンガン−亜鉛系フエライトにV2O5を適量添
加するとμi、tanδ/μiなどの弱磁界特性が改善す
ることが知られているが、この表から明らかなよ
うに、Nb2O5の添加によつてもこれに匹敵する弱
磁界特性の改善が認められる。
実施例 3
実施例1の試料5と同じ組成を用い、処理条件
を変えて、磁性材料を製造し、その磁芯特性を測
定した。その結果を第3表に示す。この際使用し
た処理条件は次のとおりである。
処理条件;実施例1の熱処理と同じ条件を用い
た。
処理条件;試料を大気中において900℃まで加
熱したのち、1050℃まで50℃/hrの昇温速度で
徐熱し、さらに続いて1320℃まで300℃/hrの
昇温速度で急熱した。次いで酸素0.5%を含む
窒素雰囲気中、1320℃で3時間加熱して焼結を
完了させたのち、加熱を停止して放冷し、1200
℃に達したとき、純窒素雰囲気に切り換え、室
温まで冷却した。
この処理は、安定温度までの温度曲線は処理
条件と同じであるが、徐熱後1050℃以後の安
定温度に至る雰囲気制御が省かれている点で異
なつている。
処理条件;試料を大気中において、徐熱工程を
経ずに1050℃まで加熱したのち、酸素0.5%を
含む窒素雰囲気下において、1320℃まで300
℃/hr昇温速度で急熱し、3時間この温度に保
持し、燃結を完了させる。次いで加熱を停止し
て放冷し、1200℃に達したとき、純窒素雰囲気
に切り換え、さらに室温まで冷却した。
この処理は、900℃から1050℃までの徐熱工
程を行なわない点で処理条件と異なつている。
処理条件;試料を大気中において、1320℃まで
300℃/hrの昇温速度で急熱後、酸素0.5%を含
む窒素雰囲気中で3時間加熱し、燃結を完了さ
せたのち、加熱を停止して放冷させ、1200℃に
達したとき、純窒素雰囲気に切り換え、室温ま
で冷却した。
この処理は、徐熱工程と1050℃以後の安定温
度に至る雰囲気制御を省いた点で処理条件と
異なつている。[Table] It is known that adding an appropriate amount of V 2 O 5 to manganese-zinc ferrite improves weak magnetic field characteristics such as μi and tanδ/μi, but as is clear from this table, Nb 2 O 5 Comparable improvement in weak magnetic field characteristics is also observed by adding . Example 3 Using the same composition as Sample 5 of Example 1 but changing the processing conditions, a magnetic material was manufactured and its magnetic core characteristics were measured. The results are shown in Table 3. The processing conditions used at this time were as follows. Treatment conditions: The same conditions as for the heat treatment in Example 1 were used. Processing conditions: The sample was heated to 900°C in the atmosphere, slowly heated to 1050°C at a heating rate of 50°C/hr, and then rapidly heated to 1320°C at a heating rate of 300°C/hr. Next, the sintering was completed by heating at 1320°C for 3 hours in a nitrogen atmosphere containing 0.5% oxygen, and then the heating was stopped and allowed to cool.
When the temperature was reached, the atmosphere was switched to pure nitrogen and cooled to room temperature. In this process, the temperature curve up to the stable temperature is the same as the process conditions, but the difference is that the atmosphere control to reach the stable temperature after slow heating at 1050° C. or higher is omitted. Processing conditions: The sample was heated to 1050°C in the air without an annealing process, and then heated to 1320°C for 300°C in a nitrogen atmosphere containing 0.5% oxygen.
Rapidly heat the mixture at a heating rate of °C/hr and hold at this temperature for 3 hours to complete combustion. Next, heating was stopped and allowed to cool, and when the temperature reached 1200°C, the atmosphere was switched to pure nitrogen and further cooled to room temperature. This treatment differs from the treatment conditions in that an annealing step from 900°C to 1050°C is not performed. Processing conditions: sample in the atmosphere up to 1320℃
After rapid heating at a heating rate of 300°C/hr, heating in a nitrogen atmosphere containing 0.5% oxygen for 3 hours to complete combustion, heating was stopped and allowed to cool until it reached 1200°C. Then, the atmosphere was changed to pure nitrogen and cooled to room temperature. This treatment differs from the treatment conditions in that the annealing step and the atmosphere control to reach a stable temperature of 1050° C. or higher are omitted.
【表】
この表から明らかなように、B−H特性及び高
周波、高磁束密度、高温領域における電力損失に
ついては、処理条件の場合が最も少なく、大気
圧下における徐熱工程や酸素濃度制御を欠いた場
合には、電力損失が大きくなる。[Table] As is clear from this table, regarding B-H characteristics and power loss in high frequency, high magnetic flux density, and high temperature regions, the processing conditions have the lowest power loss, and the annealing process under atmospheric pressure and oxygen concentration control If it is missing, power loss will increase.
Claims (1)
り、原料混合物中に微量成分として酸化ニオブ又
は焼成により酸化ニオブを生じる化合物をNb2O5
換算で0.02〜0.10重量%の割合で添加したのち、
大気圧下における徐熱工程及び酸素濃度を制御し
た雰囲気下における急熱工程を経て所定の燃結温
度まで昇温させ、この温度において燃結を完了さ
せることを特徴とする、B−HループのBm/Br
が3.0以上であつて、かつ100KHz、2000G、100℃
の条件下での電力損失が450mW/c.c.以下である
磁性材料の製造方法。1. In producing manganese-zinc ferrite, niobium oxide or a compound that produces niobium oxide upon calcination is added as a trace component to the raw material mixture using Nb 2 O 5
After adding at a ratio of 0.02 to 0.10% by weight,
The B-H loop is characterized by raising the temperature to a predetermined combustion temperature through a gradual heating process under atmospheric pressure and a rapid heating process in an atmosphere with controlled oxygen concentration, and completing combustion at this temperature. Bm/Br
is 3.0 or higher, and 100KHz, 2000G, 100℃
A method for manufacturing a magnetic material that has a power loss of 450 mW/cc or less under the following conditions.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56113311A JPS5815037A (en) | 1981-07-20 | 1981-07-20 | Magnetic manganese-zinc ferrite material and its manufacture |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56113311A JPS5815037A (en) | 1981-07-20 | 1981-07-20 | Magnetic manganese-zinc ferrite material and its manufacture |
Related Child Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2255274A Division JP2532159B2 (en) | 1990-09-27 | 1990-09-27 | Transformer core for high frequency power supply |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5815037A JPS5815037A (en) | 1983-01-28 |
| JPH0353270B2 true JPH0353270B2 (en) | 1991-08-14 |
Family
ID=14609010
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56113311A Granted JPS5815037A (en) | 1981-07-20 | 1981-07-20 | Magnetic manganese-zinc ferrite material and its manufacture |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5815037A (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS62142303A (en) * | 1986-10-28 | 1987-06-25 | Sumitomo Special Metals Co Ltd | Oxide magnetic material |
| JPH0744098B2 (en) * | 1990-03-03 | 1995-05-15 | 川崎製鉄株式会社 | Low loss Mn-Zn ferrite |
| JPH0629115A (en) * | 1991-06-29 | 1994-02-04 | Hitachi Ferrite Ltd | Manufacture of very low loss ferrite |
-
1981
- 1981-07-20 JP JP56113311A patent/JPS5815037A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5815037A (en) | 1983-01-28 |
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