JPS58114401A - Superlow loss ferrite for power source - Google Patents

Superlow loss ferrite for power source

Info

Publication number
JPS58114401A
JPS58114401A JP56209625A JP20962581A JPS58114401A JP S58114401 A JPS58114401 A JP S58114401A JP 56209625 A JP56209625 A JP 56209625A JP 20962581 A JP20962581 A JP 20962581A JP S58114401 A JPS58114401 A JP S58114401A
Authority
JP
Japan
Prior art keywords
weight
cao
power loss
nb2o5
less
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
JP56209625A
Other languages
Japanese (ja)
Other versions
JPH0463526B2 (en
Inventor
Akira Morita
守田 章
Tadakatsu Sano
佐野 忠勝
Toshio Saito
俊夫 斉藤
Shunji Kijima
鬼島 俊二
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
TDK Corp
Original Assignee
TDK Corp
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 TDK Corp filed Critical TDK Corp
Priority to JP56209625A priority Critical patent/JPS58114401A/en
Publication of JPS58114401A publication Critical patent/JPS58114401A/en
Publication of JPH0463526B2 publication Critical patent/JPH0463526B2/ja
Granted legal-status Critical Current

Links

Classifications

    • 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
    • H01F1/342Oxides
    • H01F1/344Ferrites, e.g. having a cubic spinel structure (X2+O)(Y23+O3), e.g. magnetite Fe3O4

Landscapes

  • Chemical & Material Sciences (AREA)
  • Dispersion Chemistry (AREA)
  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Soft Magnetic Materials (AREA)

Abstract

PURPOSE:To contrive the reduction of power loss in a specific temperature region, by compositely adding a specific amount of CaO, Nb2O5 and SiO2 as the sub component to the ferrite powder of MnO, ZnO Fe2O3 as the main component. CONSTITUTION:To MnO, ZnO and Fe2O3 as the main component, CaO in 0.04- 0.2wt%, Nb2O5 in 0.1wt% or less (not including 0) and SiO2 in 0.05wt% or less (not including 0) are added as the sub component so that they are contained. When CaO becomes more than 0.2wt%, a ferrite sintered body with the lack of sintering is formed, and, when less than 0.04wt%, the natural resistance of the sintered body decreases too much resulting in the deterioration of the frequency characteristic. When Nb2O5 becomes more than 0.1wt%, an inhomogeneous crystal grain growth is caused resulting in the deterioration of te magnetic characteristic, and, when SiO2 becomes more than 0.05wt%, likewise, the magnetic characteristic deteriorates. Thereby, the power loss before and after 60- 80 deg.C can be extremely reduced.

Description

【発明の詳細な説明】 本発明は、DC−DCコンバータ装置(高周波電源)の
磁芯等に用いるのに適したMrrZn系の電源用超低損
失7エライトに関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to MrrZn-based ultra-low loss 7-elite for power supplies suitable for use in magnetic cores of DC-DC converter devices (high frequency power supplies).

従来のMn−Zn系フェライトとしては、CaOとS 
i O2とを添加したものやNb2O,を単独添加した
ものがあった。しかし、そのような従来のフェライトで
はDC−DCコンバータの如く使用時の磁束密度が大で
発熱を伴う場合には電力損失が大きくなるきらいがあっ
た。
Conventional Mn-Zn ferrites include CaO and S.
There were those to which Nb2O was added and those to which Nb2O was added alone. However, such conventional ferrite tends to cause large power loss when used in a DC-DC converter where the magnetic flux density is high and heat is generated.

本発明は、上記の点に鑑み、60〜80°C前後におけ
る電力損失を極めて小さくすることが可能な電源用超低
損失7エライトを提供りようとするものである。
In view of the above-mentioned points, the present invention aims to provide an ultra-low loss 7ELITE for power supply that can extremely reduce power loss at around 60 to 80°C.

本発明の特徴は、MnO,ZnO,Fe2O,を主成分
としたラエライト粉体に副成分としてCa Oを0.0
4〜0.2重量%、Nb、O,を0を含まず0.1重量
%以下でかっ5in2を0を含まず0.05%重量重量
%以下撚加含有して本焼成したことにある。
The feature of the present invention is that 0.0% of CaO is added as a subcomponent to laerite powder mainly composed of MnO, ZnO, and Fe2O.
4 to 0.2% by weight, Nb, O, not including 0 and not more than 0.1% by weight, and 5in2 which does not contain 0 and not more than 0.05% by weight and is twisted and fired. .

以下、本発明に係る電源用超低損失フェライトの実施例
を比較例とともに説明する。
Examples of the ultra-low loss ferrite for power supplies according to the present invention will be described below along with comparative examples.

r比較例1]  Mn0(35,5モル%)、Zn0(
11,5モル%)、Fe20s (53,0%)を主成
分とし、副成分としでCaOを0.04重量%及びSi
O2を0.018重量%含有するように添加したときの
正弦波25kHz、2000fウスの條件下における8
0℃の電力損失は178mW/co+3であった。
r Comparative Example 1] Mn0 (35.5 mol%), Zn0 (
11.5 mol%), Fe20s (53.0%) as the main component, and 0.04% by weight of CaO and Si as secondary components.
8 under the conditions of a 25 kHz sine wave and 2000 fus when O2 was added to contain 0.018% by weight.
The power loss at 0° C. was 178 mW/co+3.

[比較例2’l  ’Mn0(35,5モル%)、Zn
0(11,5モル%)、Fe2O,(53,0%)を主
成分とし、!i11成分としてCaOをO,’075重
量%及び5in2を0.018重量%含有するように添
加したときの 80°Cにおける電力損失は74III
W/c−3であった。なお、この測定條件は[比較例1
]と同じである。(以下間−條件で測定した。)[実施
例1]  Mn0(35,5モル%)、Zn0(11,
5モル%)、Fe2e3(53,0%)を主成分とし、
副成分としてCa Oを0.075重量%、Nb2O,
を0.03重量%及ヒS i O、ヲ0.021重量%
含有するように添加したときの80’Cにおける電力損
失は43 mW/ca+’であった。また、この場合常
温での初透磁率μ;は2300.Qは110、jan(
δ/μ1)=3.95X10−’であり、キューリ一温
度は22o°であった。この温度は電源用として充分高
いものである。
[Comparative Example 2'l'Mn0 (35.5 mol%), Zn
0 (11.5 mol%), Fe2O, (53.0%) as the main components,! The power loss at 80°C when CaO was added as the i11 component to contain 0.075% by weight and 0.018% by weight of 5in2 was 74III.
It was W/c-3. Note that this measurement condition is [Comparative Example 1]
] is the same as (Measured under the following conditions.) [Example 1] Mn0 (35.5 mol%), Zn0 (11,
5 mol%), Fe2e3 (53.0%) as the main component,
0.075% by weight of CaO, Nb2O,
0.03% by weight and 0.021% by weight of SiO.
The power loss at 80'C when added to contain was 43 mW/ca+'. In this case, the initial magnetic permeability μ at room temperature is 2300. Q is 110, jan(
δ/μ1)=3.95×10−′, and the Curie temperature was 22°. This temperature is high enough for power supply.

[実施例2]  Mn0(35,5モル%)、Zn0(
11,5モル%)、Fe20a (53、0%)を主成
分とし、副成分としてCa Oを0.075重量%、N
b2O5を0.05重量%及C/ S + 02 全0
0olBfi量%含有するように添加したときの80″
Cにおける電力損失は64IIIW/CIs:Iであっ
た。
[Example 2] Mn0 (35.5 mol%), Zn0 (
11.5 mol%), Fe20a (53.0%) as the main component, CaO as the subcomponent 0.075% by weight, N
b2O5 0.05% by weight and C/S+02 Total 0
80″ when added to contain 0olBfi amount%
The power loss in C was 64IIIW/CIs:I.

[実施例3]  Mn0(35,5モル%)、Zn0(
11,5,モル%)、Fe2es (53,0%)を主
成分とし、副成分としてCa Oを0.075重量%、
Nb2O5を0.02重量%及びSiO2を0.018
重量%含有するように添加したときの80°Cにおける
電力損失は68 mW/Cm’であった。
[Example 3] Mn0 (35.5 mol%), Zn0 (
11,5, mol%), Fe2es (53,0%) as the main component, CaO as a subcomponent 0.075% by weight,
0.02% by weight of Nb2O5 and 0.018% of SiO2
The power loss at 80°C was 68 mW/Cm' when it was added to contain % by weight.

上記比較例及び本発明の実施例の添加物と電力損失との
関係をまとめると以下の表1の如くなる。
The relationship between additives and power loss in the comparative examples and examples of the present invention is summarized in Table 1 below.

表1 (重量%)        (論W /c論3)この表
1より本発明の実施例1,2.3の場合、比較例1,2
よりもかなり80°、Cでの電力損失が減少することが
判る。
Table 1 (wt%) (Theory W/c Theory 3) From this table 1, in the case of Examples 1 and 2.3 of the present invention, Comparative Examples 1 and 2
It can be seen that the power loss at 80°C is significantly reduced.

次に各添加物の添加量と電力損失との関係を第1図及び
第2図に示す。
Next, the relationship between the amount of each additive added and power loss is shown in FIGS. 1 and 2.

第1図は5in2を0.021重量%としN b 20
 sの添加量をパラメータとしたときの80°Cでの電
力損失に対するC a Oの添加効果を示す。図中曲線
(イ)はN b 20 sが0の場合、(ロ)は0.0
2重量%の場合、(ハ)は0.03重量%の場合である
。この図からNb2O5が添加されておりかつCaOが
0.04重量%以上であれば、かなり電力損失が減少す
ることが判る。なお、CaOが0.2重量%より多くな
ると焼結不足のフェライト焼結体となってしまうので好
ましくない。
In Figure 1, 5in2 is 0.021% by weight and N b 20
The effect of addition of C a O on power loss at 80° C. is shown when the amount of addition of s is used as a parameter. In the figure, curve (a) is 0.0 when N b 20 s is 0.
In the case of 2% by weight, (c) is the case of 0.03% by weight. From this figure, it can be seen that when Nb2O5 is added and CaO is 0.04% by weight or more, the power loss is considerably reduced. It should be noted that if the CaO content exceeds 0.2% by weight, the ferrite sintered body will be insufficiently sintered, which is not preferable.

第2図はCaOを0.075重量%としS i O2を
パラメータとしたと鰺のNb2O5の添加効果を示す。
Figure 2 shows the effect of adding Nb2O5 to mackerel when CaO was 0.075% by weight and S i O2 was used as a parameter.

図中曲線(ニ)はS i O2が0.018重量%の場
合、(ホ)は0.021重量%、(へ)は0.025%
の場合を示す。この図から、とくにN b 20 sが
0.02〜0.05%の範囲で電力損失がかなり少なく
なる。ただし、N b 20 sが0.1重量%より多
いと不均質な結晶粒成長な招外磁気特性が悪化する。
In the figure, curve (d) is when S i O2 is 0.018% by weight, (e) is 0.021% by weight, and (f) is 0.025%.
The case is shown below. From this figure, power loss is considerably reduced especially when N b 20 s is in the range of 0.02 to 0.05%. However, if N b 20 s is more than 0.1% by weight, the induced magnetic properties such as non-uniform crystal grain growth will deteriorate.

なお、5in2も0.05重量%より多いと不均質な結
晶粒成長を招軽磁気特性が悪化する。また、Ca Oが
0.04重量%より少ないと、焼結体の固有抵抗が低く
なりすぎ周波数特性が悪化する。さらに、Nb2O,と
5in2とを添加しないときには、充分な結晶粒子が得
られず、やはり磁気特性が悪化する。
Note that if 5in2 is also more than 0.05% by weight, non-uniform crystal grain growth will occur and the light magnetic properties will deteriorate. Moreover, if CaO is less than 0.04% by weight, the specific resistance of the sintered body becomes too low and the frequency characteristics deteriorate. Furthermore, when Nb2O and 5in2 are not added, sufficient crystal grains cannot be obtained, and the magnetic properties also deteriorate.

第3図は電力損失の周波数特性であって、実線(ト)は
本発明の実施例1の場合、点線(チ)はNb、Olを添
加していない既存材(比較例1に相当)の場合を示す。
Figure 3 shows the frequency characteristics of power loss, where the solid line (G) is for Example 1 of the present invention, and the dotted line (H) is for the existing material without adding Nb and Ol (corresponding to Comparative Example 1). Indicate the case.

この図から、実用周波数範囲において実施例の方がかな
りすぐれている。
From this figure, the example is considerably superior in the practical frequency range.

第4図は電力損失の温度特性を示す。この図において、
実線(す)は実施例1の場合、点線(ヌ)は既存材の場
合である。この図から80°C前後における電力損失は
相当減少していることが判る。
FIG. 4 shows the temperature characteristics of power loss. In this diagram,
The solid line (su) is for Example 1, and the dotted line (nu) is for the existing material. It can be seen from this figure that the power loss at around 80°C is considerably reduced.

以上説明したように、本発明の電源用超低損失7ヱライ
トよれば、MnO,Zn0=Fe20−を主成分とし、
Ca Oを0.04−0.2重量%、Nb2O5を0を
含まず0.1重量%以下、かつS i O2をOを含ま
ず 0.05重量%以下を副成分として複合添加したの
で、特に60〜806C前後における電力損失を極めて
少なくすることができる。従って、DC−DCコンバー
タ用トランスの如く、使用時の磁束密度が大で発熱を伴
う磁芯に用いれば効果が大きく、同一形状で既存材のと
きより15%位出力を向上させることがでl&名。
As explained above, according to the ultra-low loss 7elite for power supply of the present invention, MnO, Zn0=Fe20- are the main components,
Since 0.04-0.2% by weight of CaO, 0.1% by weight or less of Nb2O5 and 0.05% by weight or less of SiO2 without containing O were added as subcomponents, In particular, power loss around 60 to 806C can be extremely reduced. Therefore, if used in a magnetic core that has a high magnetic flux density and generates heat during use, such as a transformer for a DC-DC converter, it will have a great effect, and the output can be improved by about 15% compared to the existing material with the same shape. given name.

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

第1図は電力損失に対するCaの添加効果を示すグラフ
、第2図はNb2O,の添加効果を示すグラフ、第3図
は電力損失の周波数特性を示すグラフ、第4図は温度特
性を示すグラフである。 特許出願人 東京電気化学工業株式会社 代理人 弁理士 村 井  隆
Figure 1 is a graph showing the effect of Ca addition on power loss, Figure 2 is a graph showing the effect of Nb2O addition, Figure 3 is a graph showing frequency characteristics of power loss, and Figure 4 is a graph showing temperature characteristics. It is. Patent applicant Tokyo Denki Kagaku Kogyo Co., Ltd. Patent attorney Takashi Murai

Claims (1)

【特許請求の範囲】[Claims] (1)  MnO,ZnO,Fe20s を主成分とし
、CaOを0.04〜0.2重量館、Nb2O5を0を
含まず0.1重量%以下、かっ5in2をOを含まず0
.05重量%以下を副成分として複合添加含有したこと
を特徴とする電源用超低損失7エライシ。
(1) The main components are MnO, ZnO, and Fe20s, CaO is 0.04 to 0.2% by weight, Nb2O5 is 0.1% by weight or less, and 5in2 is 0% without O.
.. Ultra-low loss 7 element for power supply characterized by containing 0.05% by weight or less as a composite additive as an auxiliary component.
JP56209625A 1981-12-28 1981-12-28 Superlow loss ferrite for power source Granted JPS58114401A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56209625A JPS58114401A (en) 1981-12-28 1981-12-28 Superlow loss ferrite for power source

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56209625A JPS58114401A (en) 1981-12-28 1981-12-28 Superlow loss ferrite for power source

Publications (2)

Publication Number Publication Date
JPS58114401A true JPS58114401A (en) 1983-07-07
JPH0463526B2 JPH0463526B2 (en) 1992-10-12

Family

ID=16575888

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56209625A Granted JPS58114401A (en) 1981-12-28 1981-12-28 Superlow loss ferrite for power source

Country Status (1)

Country Link
JP (1) JPS58114401A (en)

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60132301A (en) * 1983-12-20 1985-07-15 Sumitomo Special Metals Co Ltd Oxide magnetic material
JPH0230660A (en) * 1988-07-18 1990-02-01 Mitsubishi Electric Corp Low-loss magnetic material of oxide
JPH03163802A (en) * 1989-11-22 1991-07-15 Kawasaki Steel Corp Low loss mn-zn system ferrite
JPH03212906A (en) * 1990-01-18 1991-09-18 Hitachi Ferrite Ltd Manufacture of high frequency low loss ferrite for power supply
JPH03248403A (en) * 1990-02-26 1991-11-06 Hitachi Ferrite Ltd Low-loss ferrite
JPH03248405A (en) * 1990-02-26 1991-11-06 Hitachi Ferrite Ltd Low-loss ferrite for power supply
JPH03248404A (en) * 1990-02-26 1991-11-06 Hitachi Ferrite Ltd Low-loss ferrite
JPH03254103A (en) * 1990-03-03 1991-11-13 Kawasaki Steel Corp Low-loss mn-zn ferrite
JPH04336401A (en) * 1991-05-14 1992-11-24 Kawasaki Steel Corp Oxide soft magnetic material

Cited By (13)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60132301A (en) * 1983-12-20 1985-07-15 Sumitomo Special Metals Co Ltd Oxide magnetic material
JPH0521859B2 (en) * 1983-12-20 1993-03-25 Sumitomo Spec Metals
JPH0230660A (en) * 1988-07-18 1990-02-01 Mitsubishi Electric Corp Low-loss magnetic material of oxide
JPH0710744B2 (en) * 1988-07-18 1995-02-08 三菱電機株式会社 Low loss oxide magnetic material
JPH03163802A (en) * 1989-11-22 1991-07-15 Kawasaki Steel Corp Low loss mn-zn system ferrite
JPH03212906A (en) * 1990-01-18 1991-09-18 Hitachi Ferrite Ltd Manufacture of high frequency low loss ferrite for power supply
JPH03248404A (en) * 1990-02-26 1991-11-06 Hitachi Ferrite Ltd Low-loss ferrite
JPH03248405A (en) * 1990-02-26 1991-11-06 Hitachi Ferrite Ltd Low-loss ferrite for power supply
JPH03248403A (en) * 1990-02-26 1991-11-06 Hitachi Ferrite Ltd Low-loss ferrite
JPH03254103A (en) * 1990-03-03 1991-11-13 Kawasaki Steel Corp Low-loss mn-zn ferrite
US5143638A (en) * 1990-03-03 1992-09-01 Kawasaki Steel Corporation Low power loss mn-zn ferrites
US5368763A (en) * 1990-03-03 1994-11-29 Kawasaki Steel Corporation Low power loss Mn-Zn ferrites
JPH04336401A (en) * 1991-05-14 1992-11-24 Kawasaki Steel Corp Oxide soft magnetic material

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