JPH03248405A - Low-loss ferrite for power supply - Google Patents

Low-loss ferrite for power supply

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Publication number
JPH03248405A
JPH03248405A JP2048714A JP4871490A JPH03248405A JP H03248405 A JPH03248405 A JP H03248405A JP 2048714 A JP2048714 A JP 2048714A JP 4871490 A JP4871490 A JP 4871490A JP H03248405 A JPH03248405 A JP H03248405A
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JP
Japan
Prior art keywords
less
low
loss
mno
zno
Prior art date
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Granted
Application number
JP2048714A
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Japanese (ja)
Other versions
JP3044666B2 (en
Inventor
Tokukazu Koyuhara
徳和 小湯原
Hitoshi Ueda
等 上田
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Proterial Ltd
Original Assignee
Hitachi Ferrite Ltd
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  • Soft Magnetic Materials (AREA)

Abstract

PURPOSE:To obtain a ferrite with a low power loss featuring a high magnetic flux density over a frequency range of 25-1MHz by adding and including Fe2O3, MnO, and ZnO as main constituents and a specific amount of CaO, SiO2, Nb2O5, and Ta2O5 compositely as a sub-constituent. CONSTITUTION:Fe2O3, MnO, and ZnO are included as main constituents and 200-1000ppm CaO, 500ppm or less SiO2, 1500ppm or less Nb2O5, and 1500ppm or less Ta2O5 (none of these includes 0) are added and included compositely. After a raw material whose main constituents are Fe2O3, MnO, and ZnO is tentatively baked, CaCO3, SiO2, Nb2O5, and Ta2O5 are added compositely and are ground by a ball mill. After this ground raw material is dried, a binder is added to enable a grain to be formed, forming to be performed, and baking to be made.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、スイッチング電源の磁心等に用いるのに適し
たMn−Zn系の低損失フェライトに関するもので、C
ab、Sin、 、Nb、O3,Ta、Osもしくは、
 Cab、5i02、Nb、O3,Ta、Os ,Ti
O、もしくは、Cab、Sin、 、Nb、0. 。
Detailed Description of the Invention (Field of Industrial Application) The present invention relates to a Mn-Zn-based low-loss ferrite suitable for use in magnetic cores of switching power supplies, etc.
ab, Sin, , Nb, O3, Ta, Os or
Cab, 5i02, Nb, O3, Ta, Os, Ti
O, or Cab, Sin, , Nb, 0. .

Tie、を微量複合添加することにより25kHz〜I
 MHzにおける電力損失を著しく低減したものである
25kHz~I by adding a small amount of Tie.
This significantly reduces power loss at MHz.

(従来の技術) Mn−Zn系の低損失フェライトは、各種通信機器、民
生用機器などのトランス用材料に用いられているが、従
来のスイッチング電源用トランスにおいては、スイッチ
ング周波数として専ら25〜200kHz程度のものが
使用されている。このスイッチング電源用トランスに用
いられる低損失フェライトとしては、副成分として、C
aO、Sin、 、 V2O,を含む、あるいはCaO
H5io2t Nbz Osを含む所望のMn−Zn系
フェライトが使用されている。例えば、特開昭58−1
14401号公報。
(Prior art) Mn-Zn-based low-loss ferrites are used as materials for transformers in various communication devices, consumer devices, etc., but in conventional transformers for switching power supplies, the switching frequency is exclusively 25 to 200 kHz. A certain amount is used. The low-loss ferrite used in this switching power supply transformer contains C as a subcomponent.
Contains aO, Sin, , V2O, or CaO
Desired Mn-Zn based ferrites including H5io2tNbzOs are used. For example, JP-A-58-1
Publication No. 14401.

(発明が解決しようとする問題点) 近年−、スイッチング電源をさらに小型・軽量化、高周
波化するため、これに使用するフェライト材料としても
、使用周波数領域において、より低損失で、より高磁束
密度の材料が必要不可欠となっている。
(Problem to be solved by the invention) In recent years, in order to make switching power supplies even smaller, lighter, and capable of higher frequencies, ferrite materials used for these power supplies have lower loss and higher magnetic flux density in the operating frequency range. materials are indispensable.

しかし、従来のMn−Zn系フェライトでは、高磁束密
度で、なおかつ低損失の共有を実現することは容易でな
かった。また、数百kHz以上の周波数領域では、電力
損失が増大してしまう欠点があった。 本発明は1周波
数25〜200kHzにおいて、あるいは、周波数20
0kHz〜I MHzにおいて、高磁束密度で、なおか
つ充分電力損失の少ない電源用低損失フェライトを提供
しようとするものである。
However, with conventional Mn--Zn-based ferrites, it has not been easy to achieve high magnetic flux density and low loss sharing. Furthermore, there is a drawback that power loss increases in a frequency range of several hundred kHz or more. The present invention can be applied at a frequency of 25 to 200kHz or at a frequency of 20kHz.
The present invention aims to provide a low-loss ferrite for power supplies that has a high magnetic flux density and sufficiently low power loss in the range from 0 kHz to I MHz.

(問題点を解決するための手段) 本発明は、 Fe2O3,MnO,Zr+0を主成分と
し、副成分として、 1) CaO200〜11000pp、Si0□500
ppm以下(0を含まず)、Nb2051500pp+
m以下(0を含まず)tTazos 1500ppm以
下(0を含まず) 2) CaO200〜1OOOpp+m、SL0.50
0pp+i以下(0を含まず)+Nb2O51500p
pm以下(0を含まず)lTa、0.1500ρp@以
下(0を含まず)、T1011000〜20000pρ
−3) CaO200〜11000pp、SS1025
00pp以下(0を含まず)、Nb、0.1500pp
m以下(0を含まず)、TiO□1000〜20000
ppm を複合添加、含有することにより、25kHz〜I M
Hzにおいて、高磁束密度で、なおかつ、充分電力損失
の少ないフェライトを得るものである。
(Means for solving the problems) The present invention has Fe2O3, MnO, and Zr+0 as main components, and as subcomponents: 1) CaO200-11000pp, Si0□500
ppm or less (not including 0), Nb2051500pp+
m or less (not including 0) tTazos 1500 ppm or less (not including 0) 2) CaO200~1OOpp+m, SL0.50
0pp+i or less (not including 0)+Nb2O51500p
pm or less (not including 0) lTa, 0.1500ρp@ or less (not including 0), T1011000~20000pρ
-3) CaO200-11000pp, SS1025
00pp or less (not including 0), Nb, 0.1500pp
m or less (not including 0), TiO□1000-20000
By adding and containing ppm in combination, 25kHz to IM
The present invention aims to obtain a ferrite having a high magnetic flux density and sufficiently low power loss at Hz.

(実施例) 以下本発明に関する電源用低損失フェライトの実施例を
説明する。
(Example) An example of a low-loss ferrite for power supply according to the present invention will be described below.

(1) Fsz03(53mo1%)、Mn0(35,
5mo1%)、Zn0(11,5mo1%)を主成分と
する原料を900℃にて仮焼成した後。
(1) Fsz03 (53mo1%), Mn0 (35,
5 mo1%) and Zn0 (11.5 mo1%) after pre-calcining at 900°C.

副成分として、CaCO3を750ppm(CaOに換
算すると420ppm) 、5in2を50ppm、N
b、O,を700ppm,Ta、O,を1100pp複
合添加し、ボールミルにて2時間粉砕した。
As subcomponents, 750 ppm of CaCO3 (420 ppm when converted to CaO), 50 ppm of 5in2, N
700 ppm of b, O, and 1100 ppm of Ta and O were added in combination, and the mixture was ground in a ball mill for 2 hours.

但し、Cab、Sin、にょうに原料に予め含有されて
いる副成分については、仮焼成後に添加する量をその分
だけ減じ、全体として上記成分の割合に一致する様にし
た。
However, for the subcomponents previously contained in the raw materials such as Cab, Sin, and Nyon, the amounts added after pre-calcination were reduced by that amount, so that the overall proportions matched the above-mentioned component proportions.

この粉砕原料を乾燥後、バインダーを1wt%添加し、
造粒、成形した。この成形体を焼成温度1300℃、焼
成雰囲気は酸素分圧1%にて5時間焼成した。なお、焼
成体の形状は、外径30■、内径20■。
After drying this pulverized raw material, 1 wt% of binder was added,
Granulated and molded. This molded body was fired for 5 hours at a firing temperature of 1300° C. and a firing atmosphere of 1% oxygen partial pressure. The shape of the fired body is 30 cm in outer diameter and 20 cm in inner diameter.

高さ10IImのリング状とした。It was made into a ring shape with a height of 10 IIm.

この実施例1と同様の試料作製工程において。In the sample preparation process similar to this Example 1.

添加物条件を変えて各試料を作製した。この結果を第1
表に示す。
Each sample was prepared with different additive conditions. This result is the first
Shown in the table.

第 表 試料1〜6,8〜11は、周波数25〜200kHzに
おいて、電力損失の少ない本発明の実施例であり、試料
7は、添加物としてCab、Sin、 、Nb2O,を
含む従来材の例である。
Samples 1 to 6 and 8 to 11 in the table are examples of the present invention with low power loss at frequencies of 25 to 200 kHz, and sample 7 is an example of a conventional material containing Cab, Sin, , Nb2O, as additives. It is.

実施例6の電力損失の温度特性を第1図に、また、電力
損失の周波数特性を第2図に示した。なお、比較例とし
て従来例の電力損失の温度特性及び周波数特性も第1図
及び第2図に示した。
The temperature characteristics of power loss in Example 6 are shown in FIG. 1, and the frequency characteristics of power loss are shown in FIG. As a comparative example, the temperature characteristics and frequency characteristics of the power loss of the conventional example are also shown in FIGS. 1 and 2.

第1図より、実施例6の電源用低損失フェライトは、周
波数f=100kHz、磁束密度B+i=200mTに
おいて、20℃〜120℃の広温度範囲で電力損失が従
来材の7割程度と、極めて低いことがわかる。また、第
1表に示した様に各実施例の飽和磁束密度は、510m
T以上と非常に高く、このため、第2図に示した様な優
れた電力損失の周波数特性が得られた。
From Figure 1, the low-loss ferrite for power supply of Example 6 has an extremely low power loss of about 70% of that of conventional materials over a wide temperature range of 20°C to 120°C at a frequency f = 100kHz and a magnetic flux density B+i = 200mT. You can see that it is low. In addition, as shown in Table 1, the saturation magnetic flux density of each example was 510 m
This is very high, more than T, and therefore excellent frequency characteristics of power loss as shown in FIG. 2 were obtained.

また、実施例6以外の本発明の電源用低損失フェライト
(実施例1〜10)においても、第2図に示したものと
同様の傾向が見られた。
Furthermore, the same tendency as shown in FIG. 2 was observed in the low-loss ferrites for power supplies of the present invention (Examples 1 to 10) other than Example 6.

(2) Fe2O,(53,5mo1%)、Mn0(3
7,5mo1%)、Zn0(9,Omo1%)を主成分
とする原料を900℃にて仮焼成した後、副成分として
、CaC0,を750ppm(CaOに換算すると42
0ppm) *5x01を300ppm、NbzOsを
500pp■,Ta5O,を100pp■複合添加し、
ボールミルにて12時間粉砕した。但し、CaO,Si
O□のように原料に予め含有されている副成分について
は、仮焼成後に添加する量をその分だけ減じ、全体とし
て上記成分の割合に一致する様にした。
(2) Fe2O, (53.5mol1%), Mn0 (3
7,5mo1%), Zn0 (9,Omo1%) as the main components is calcined at 900°C, and then CaC0 is added as a subcomponent at 750ppm (42% when converted to CaO).
0ppm) *300ppm of 5x01, 500pp of NbzOs, 100pp of Ta5O were added in combination,
The mixture was ground in a ball mill for 12 hours. However, CaO, Si
Regarding subcomponents such as O□, which were previously contained in the raw materials, the amount added after the pre-calcination was reduced by that amount, so that the overall ratio matched the above-mentioned component ratio.

この粉砕原料を乾燥後、バインダーを1wt%添加し、
造粒、成形した。この成形体を焼成温度1150℃、焼
成雰囲気は酸素分圧0.1%にて5時間焼成した。なお
、焼成体の形状は、外径25■、内径15■、高さ7.
5msのリング状とした。
After drying this pulverized raw material, 1 wt% of binder was added,
Granulated and molded. This molded body was fired for 5 hours at a firing temperature of 1150° C. and a firing atmosphere of 0.1% oxygen partial pressure. The shape of the fired body is 25 cm in outer diameter, 15 cm in inner diameter, and 7 cm in height.
It was made into a ring shape with a duration of 5 ms.

この実施例15と同様の試料作製工程において、添加物
条件を変えて各試料を作製した。この結果を第2表に示
す。
In the same sample preparation process as in Example 15, each sample was prepared with different additive conditions. The results are shown in Table 2.

第 表 試料12〜22は、周波数200kHz 〜I MHz
において電力損失の少ない本発明の実施例である。
Samples 12 to 22 in the table have a frequency of 200kHz to I MHz.
This is an embodiment of the present invention in which power loss is small.

実施例15の電力損失の温度特性を第3図に、また、電
力損失の周波数特性を第4図に示した。なお、比較とし
て従来例(試料7)の電力損失の温度特性及び周波数特
性も第3図及び第4図に示した。
The temperature characteristics of power loss in Example 15 are shown in FIG. 3, and the frequency characteristics of power loss are shown in FIG. For comparison, the temperature characteristics and frequency characteristics of power loss of the conventional example (sample 7) are also shown in FIGS. 3 and 4.

第3図より、実施例15の電源用低損失フェライトは、
周波数f=500kHz、磁束密度Bm:50+mTに
おいて、20℃〜120℃の広温度範囲で電力損失が従
来材の1/2〜l/3程度と、極めて低いことがわかる
From FIG. 3, the low-loss ferrite for power supply of Example 15 is
It can be seen that at a frequency f=500 kHz and a magnetic flux density Bm of 50+mT, the power loss is extremely low at about 1/2 to 1/3 of that of conventional materials over a wide temperature range of 20° C. to 120° C.

また、第4図より、実施例15の電源用低損失フェライ
トが、従来の電源用フェライトに比べ、損失が172と
なるのは、磁束密度50■Tでは200kHz以上10
0mTでは、 300kHz以上であり、200mTで
は、I N)Iz以上であることが予想される。すなわ
ち。
Moreover, from FIG. 4, the loss of the low-loss ferrite for power supply of Example 15 is 172 compared to the conventional ferrite for power supply, because the loss is 172 at a magnetic flux density of 50 T and above 200 kHz.
At 0 mT, it is expected to be at least 300 kHz, and at 200 mT, it is expected to be at least IN)Iz. Namely.

実施例15が高周波低損失という特徴を発揮するのは、
周波数200kHz以上、磁束密度100■T以下の動
作条件であると言える。
The reason why Embodiment 15 exhibits the characteristic of low loss at high frequencies is because
It can be said that the operating conditions are a frequency of 200kHz or more and a magnetic flux density of 100T or less.

また、実施例15以外の本発明の電源用低損失フェライ
ト(実施例11〜21)においても、第4図に示したも
のと同様の傾向が見られた。
Furthermore, the same tendency as shown in FIG. 4 was observed in the low-loss ferrites for power supplies (Examples 11 to 21) of the present invention other than Example 15.

尚、主成分である。 Fe、O3,MnO,ZnOの割
合は、Fe、0. 52.0〜55.Omo1%、Mn
0 31.0〜42.0mo1%、  ZnO6,0〜
16.0mo1%の範囲であれば良い。
Note that this is the main component. The proportions of Fe, O3, MnO, and ZnO are as follows: Fe, 0. 52.0-55. Omo1%, Mn
0 31.0~42.0mo1%, ZnO6,0~
It is sufficient if it is within the range of 16.0mo1%.

また、本発明において、副成分の添加量を限定した理由
は、以下の通りである。
Further, in the present invention, the reason why the amount of the subcomponents added is limited is as follows.

副成分のCaOが11000ppより多いと、電力損失
が増大すると共に、透磁率が急激に低下する。また、C
aOが200ppmよりも少ないと、電気抵抗が低下す
るため、渦電流損失が増大し、電力損失は大きくなる。
If the subcomponent CaO is more than 11,000 pp, power loss increases and magnetic permeability rapidly decreases. Also, C
When aO is less than 200 ppm, electrical resistance decreases, eddy current loss increases, and power loss increases.

副成分のNb2O3,Ta、0. 、Sin、が本発明
の範囲以上になると、異常焼結し、電力損失が増大する
と共に、透磁率及びQ値も低下する。尚、高磁束密度・
低損失のフェライト焼結体を得るためには、SiO□添
加量は、周波数25kHz 〜200k)Iz対応のも
ので200ppm以下、周波数200kHz〜I MH
z対応のもので200〜500Pρ履の範囲で含有され
ることが望ましい。
Subcomponents Nb2O3, Ta, 0. , Sin, exceeds the range of the present invention, abnormal sintering occurs, power loss increases, and magnetic permeability and Q value also decrease. In addition, high magnetic flux density
In order to obtain a ferrite sintered body with low loss, the amount of SiO□ added must be 200 ppm or less for frequencies of 25 kHz to 200 kHz, and 200 ppm or less for frequencies of 200 kHz to IMH.
It is desirable that the content is in the range of 200 to 500 Pρ for Z-compatible.

また、副成分のNb、 O3,Ta20S及び5un2
が本発明の範囲未満になると、電気抵抗が低下し電力損
失が増大すると共に、焼結が進まず、飽和磁束密度及び
透磁率も低下する。
In addition, the subcomponents Nb, O3, Ta20S and 5un2
If it is less than the range of the present invention, electrical resistance decreases, power loss increases, sintering does not proceed, and saturation magnetic flux density and magnetic permeability also decrease.

副成分のTie2が本発明の範囲以上になると、電力損
失の温度特性の極小点が低温側にシフトし。
When the subcomponent Tie2 exceeds the range of the present invention, the minimum point of the temperature characteristic of power loss shifts to the low temperature side.

使用温度での電力損失が増大するため望ましくない。This is undesirable because it increases power loss at operating temperatures.

また、副成分のTie、が本発明の範囲未満になると電
力損失が増大すると共に、飽和磁束密度も低下するため
望ましくない。
Furthermore, if the subcomponent Tie falls below the range of the present invention, power loss increases and the saturation magnetic flux density also decreases, which is not desirable.

(発明の効果) 前述の如く、本発明の電源用低損失フェライトは.Fe
、03.MnO,ZnOを主成分とし、副成分として1
) CaO200〜11000pp、SS102500
pp以下(0を含まず)yNbzos 1500PP”
以下(0を含まず),Ta2O51500ppm以下(
0を含まず) 2) CaO200−1000ppm、SL02500
ppm以下(0を含まず)、Nb2O51500pp+
m以下(0を含まず),Ta、0.1500ppm以下
(0を含まず)、TiO□1000〜20000pp1
13) CaO200〜11000ppm,SiO2,
500ppm以下(0を含まず)Nb、Os1500p
pm以下(0を含まず),TiO、 1000〜200
00pP膳 のいずれかを複合添加、含有することにより、25kH
z〜I MHzにおいて、高磁束密度で、なおかつ充分
電力損失の少ないフェライトを得ることができる。
(Effects of the Invention) As mentioned above, the low-loss ferrite for power supplies of the present invention is... Fe
, 03. The main components are MnO and ZnO, and 1 as a subcomponent.
) CaO200-11000pp, SS102500
PP or less (not including 0)yNbzos 1500PP”
Below (not including 0), Ta2O5 below 1500ppm (
0) 2) CaO200-1000ppm, SL02500
ppm or less (not including 0), Nb2O51500pp+
m or less (not including 0), Ta, 0.1500 ppm or less (not including 0), TiO□1000-20000 pp1
13) CaO200-11000ppm, SiO2,
500ppm or less (not including 0) Nb, Os1500p
pm or less (not including 0), TiO, 1000-200
By adding and containing any of the 00pP meals, 25kHz
z~I MHz, it is possible to obtain ferrite with high magnetic flux density and sufficiently low power loss.

【図面の簡単な説明】[Brief explanation of drawings]

第1図は、本発明に係る実施例6の場合の周波数100
kHz、磁束密度200mTにおける電力損失の温度特
性を従来例の場合と比較して示したものであり、第2図
は、磁束密度200mT、周囲温度100℃における本
発明に係る実施例6の電力損失の周波数特性を従来例の
場合と比較して示したものであり、第3図は、本発明に
係る実施例15の場合の周波数500kHz、磁束密度
50mTにおける電力損失の温度特性を従来例の場合と
比較して示したものであり、第4図は、磁束密度50璽
T400mT・200鳳T、周囲温度80℃における本
発明に係る実施例15の電力損失の周波数特性を従来例
の場合と比較して示したものである。
FIG. 1 shows a frequency of 100 in the case of Example 6 according to the present invention.
The temperature characteristics of power loss at a magnetic flux density of 200 mT and a magnetic flux density of 200 mT are shown in comparison with that of a conventional example. Figure 2 shows the power loss of Example 6 according to the present invention at a magnetic flux density of 200 mT and an ambient temperature of 100°C. Figure 3 shows the frequency characteristics of power loss at a frequency of 500 kHz and magnetic flux density of 50 mT in the case of Example 15 according to the present invention in comparison with that of the conventional example. Figure 4 compares the frequency characteristics of the power loss of Example 15 according to the present invention with the conventional example at a magnetic flux density of 50T, 400mT, 200T and an ambient temperature of 80°C. This is what was shown.

Claims (3)

【特許請求の範囲】[Claims] 1.Fe_2O_3,MnO,ZnOを主成分とし、副
成分として、CaO200〜1000ppm,SiO_
2,500ppm以下(0を含まず),Nb_2O_5
1500ppm以下(0を含まず),Ta_2O_51
500ppm以下(0を含まず)を複合添加、含有した
ことを特徴とする電源用低損失フェライト。
1. The main components are Fe_2O_3, MnO, and ZnO, and the subcomponents are CaO200-1000ppm, SiO_
2,500 ppm or less (not including 0), Nb_2O_5
1500ppm or less (not including 0), Ta_2O_51
A low-loss ferrite for power supplies characterized by containing 500 ppm or less (excluding 0) in a composite manner.
2.Fe_2O_3,MnO,ZnOを主成分とし、副
成分として、CaO200〜1000ppm,SiO_
2500ppm以下(0を含まず),Nb_2O_51
500ppm以下(0を含まず),Ta_2O_515
00ppm以下(0を含まず),TiO_21000〜
20000ppmを複合添加、含有したことを特徴とす
る電源用低損失フェライト。
2. The main components are Fe_2O_3, MnO, and ZnO, and the subcomponents are CaO200-1000ppm, SiO_
2500ppm or less (not including 0), Nb_2O_51
500ppm or less (not including 0), Ta_2O_515
00ppm or less (not including 0), TiO_21000~
A low-loss ferrite for power supplies characterized by containing 20,000 ppm of compound additives.
3.Fe_2O_3,MnO,ZnOを主成分とし、副
成分として、CaO200〜1000ppm,SiO_
2500ppm以下(0を含まず),Nb_2O_51
500ppm以下(0を含まず),TiO_21000
〜20000ppmを複合添加、含有したことを特徴と
する電源用低損失フェライト。
3. The main components are Fe_2O_3, MnO, and ZnO, and the subcomponents are CaO200-1000ppm, SiO_
2500ppm or less (not including 0), Nb_2O_51
500ppm or less (not including 0), TiO_21000
A low-loss ferrite for power supplies characterized by containing ~20,000 ppm of composite additives.
JP2048714A 1990-02-26 1990-02-26 Low loss ferrite for power supply Expired - Lifetime JP3044666B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2048714A JP3044666B2 (en) 1990-02-26 1990-02-26 Low loss ferrite for power supply

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2048714A JP3044666B2 (en) 1990-02-26 1990-02-26 Low loss ferrite for power supply

Publications (2)

Publication Number Publication Date
JPH03248405A true JPH03248405A (en) 1991-11-06
JP3044666B2 JP3044666B2 (en) 2000-05-22

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Application Number Title Priority Date Filing Date
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Country Status (1)

Country Link
JP (1) JP3044666B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6627103B2 (en) 2000-03-31 2003-09-30 Tdk Corporation Mn-Zn ferrite production process, Mn-Zn ferrite, and ferrite core for power supplies

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58114401A (en) * 1981-12-28 1983-07-07 Tdk Corp Superlow loss ferrite for power source
JPS60132301A (en) * 1983-12-20 1985-07-15 Sumitomo Special Metals Co Ltd Oxide magnetic material
JPS60262405A (en) * 1984-06-11 1985-12-25 Sumitomo Special Metals Co Ltd Manufacture of mn-zn ferrite
JPH03248404A (en) * 1990-02-26 1991-11-06 Hitachi Ferrite Ltd Low-loss ferrite

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58114401A (en) * 1981-12-28 1983-07-07 Tdk Corp Superlow loss ferrite for power source
JPS60132301A (en) * 1983-12-20 1985-07-15 Sumitomo Special Metals Co Ltd Oxide magnetic material
JPS60262405A (en) * 1984-06-11 1985-12-25 Sumitomo Special Metals Co Ltd Manufacture of mn-zn ferrite
JPH03248404A (en) * 1990-02-26 1991-11-06 Hitachi Ferrite Ltd Low-loss ferrite

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6627103B2 (en) 2000-03-31 2003-09-30 Tdk Corporation Mn-Zn ferrite production process, Mn-Zn ferrite, and ferrite core for power supplies

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