JPS61252609A - Magnetic material of low-loss oxide - Google Patents
Magnetic material of low-loss oxideInfo
- Publication number
- JPS61252609A JPS61252609A JP60092205A JP9220585A JPS61252609A JP S61252609 A JPS61252609 A JP S61252609A JP 60092205 A JP60092205 A JP 60092205A JP 9220585 A JP9220585 A JP 9220585A JP S61252609 A JPS61252609 A JP S61252609A
- Authority
- JP
- Japan
- Prior art keywords
- oxide
- loss
- low
- weight
- magnetic material
- 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.)
- Pending
Links
Landscapes
- Magnetic Ceramics (AREA)
- Soft Magnetic Materials (AREA)
Abstract
Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、低損失酸化物磁性材料に関し、特に。[Detailed description of the invention] [Industrial application field] The present invention relates to low loss oxide magnetic materials, and more particularly.
主成分として30〜37モルチの一酸化マンガン(Mn
O) 、 10〜15モルチの酸化亜鉛(ZnO)及び
残部酸化第二鉄(Fe12O3 )を含み、副成分とし
て0.04〜0.10重量%の酸化カルシウム(Cab
)と0.015〜0.100重量−の二酸化ケイ素(S
102)を含む低損失酸化物磁性材料の改良に関するも
のである。The main component is 30 to 37 molt manganese monoxide (Mn).
O), containing 10 to 15 moles of zinc oxide (ZnO) and the balance ferric oxide (Fe12O3), and 0.04 to 0.10% by weight of calcium oxide (Cab) as an accessory component.
) and 0.015 to 0.100% by weight of silicon dioxide (S
This invention relates to improvements in low-loss oxide magnetic materials including 102).
従来、スイッチング電源用の変圧器においては。 Conventionally, in transformers for switching power supplies.
スイッチング周波数として専ら100 kHz程度のも
のが使用されておシ、これに対応すべき低損失酸化物磁
性材料として、上述した成分のものがすでに開発されて
いる。A switching frequency of approximately 100 kHz is used, and low-loss oxide magnetic materials having the above-mentioned components have already been developed to accommodate this.
近年、スイッチング電源を小形、軽量化するために、ス
イッチング周波数が2O0 kHz以上の高周波で使用
する要望が高まりている。ところが。In recent years, in order to make switching power supplies smaller and lighter, there has been an increasing demand for them to be used at high switching frequencies of 200 kHz or higher. However.
従来の成分を有する低損失酸化物磁性材料をスイッチン
グ周波数が2O0 kHz以上のスイッチング電源用の
変圧器の磁芯材料として使用すると、その鉄損が大きく
発熱するという欠点があった。When a low-loss oxide magnetic material having conventional components is used as a core material of a transformer for a switching power supply with a switching frequency of 200 kHz or more, there is a drawback that the core loss is large and heat is generated.
従って、一本発明の目的は0周波数が2O0 kHz〔
問題点を解決するための手段〕
本発明は、主成分として30〜37モルチのモル化マン
ガン(MnO)、・10〜15モルチのモル亜鉛(Zn
O)及び残部酸化第二鉄(Fe2O3)を含み、副成分
として0.04〜0.10重量%の酸化カルシウム(C
aO)と0.015〜0.100重量%の二酸化ケイ素
(SiO2)を含む低損失酸化物磁性材料において、
0.50〜0.90重量%の酸化第二スズ(SnO2)
を添加したことを特徴とする。Therefore, one object of the present invention is to reduce the zero frequency to 200 kHz [
Means for Solving the Problems] The present invention uses 30 to 37 mol of manganese (MnO) and 10 to 15 mol of zinc (ZnO) as main components.
O) and the balance ferric oxide (Fe2O3), and 0.04 to 0.10% by weight of calcium oxide (C
aO) and 0.015 to 0.100% by weight of silicon dioxide (SiO2),
0.50-0.90% by weight of stannic oxide (SnO2)
It is characterized by the addition of.
以下1本発明の実施例について図面を参照して説明する
。An embodiment of the present invention will be described below with reference to the drawings.
第1図は主成分として52.5モル−〇酸化第二鉄(F
e2O3) 、34.0モル係の一酸化マンガン(Mn
O)及び13.5モル係の酸化亜鉛(ZnO)を含有し
、副成分として0.018重量%の二酸化ケイ素(Si
O2)と0.045重量%の酸化カルシウム(CaO)
を含有し、添加成分として酸化第二スズ(,5n02−
、)を添加し、これらを混合し、造粒し、成形プレスし
丸後、酸素分圧0.8at%、温度1270℃において
焼結し酸化物磁性材料を得たものに対して、酸化第二ス
ズ(5n02 、)の添加量をパラメータとしたときの
温度T〔℃〕の電力損失’P’B [kW/m3〕の関
係を示した図である。Figure 1 shows 52.5 mol of ferric oxide (F) as the main component.
e2O3), 34.0 molar manganese monoxide (Mn
ZnO) and 13.5 mol of zinc oxide (ZnO), and 0.018% by weight of silicon dioxide (Si) as an accessory component.
O2) and 0.045% by weight calcium oxide (CaO)
containing stannic oxide (,5n02-
, ) were added, mixed, granulated, molded and pressed, and then sintered at an oxygen partial pressure of 0.8 at% and a temperature of 1270°C to obtain an oxide magnetic material. FIG. 2 is a diagram showing the relationship between power loss 'P'B [kW/m3] and temperature T [°C] when the amount of ditin (5n02,) added is used as a parameter.
ここで、第1図は2周波数が2O’OkHz 、最大磁
束密度Bmが2O00Gの場合の電力損失を示している
。又、第1図において、1は酸化第二スズ(5n02
)を添加しない場合、2は0.50重量%の酸イ些第二
スズ(5n02 )を添−加した場合、3は0.75重
量%の酸化第二スズ(SnO2)を添加した場合。Here, FIG. 1 shows the power loss when the two frequencies are 2O'OkHz and the maximum magnetic flux density Bm is 2000G. In addition, in FIG. 1, 1 is stannic oxide (5n02
) is not added, 2 is when 0.50% by weight of stannic acid (5N02) is added, and 3 is when 0.75% by weight of stannic oxide (SnO2) is added.
4は0.90重量%の酸化第二スズ(SnO2)を添加
した場合、5は1.00重量%の酸化第二スズ(Sn0
2)を添加した場合の特性をそれぞれあられしている。4 is when 0.90% by weight of stannic oxide (SnO2) is added, and 5 is when 1.00% by weight of stannic oxide (SnO2) is added.
The characteristics when 2) is added are shown.
第1図よ90周波数が2O0 kHzの場合、酸化第二
スズ(5nOz )を添加しないときの電力損失pBの
最小値の温度Tは約60℃であるのに対し、酸化第二ス
ズ(5nOz )の添加量を増加するにつれて電力損失
pBの最小値の温度では低温側へ移動していくことがわ
かる。又、酸化第二スズ(SnO2)の添加量が約0.
75重量%のときに、他の添加量(0俤を含む)の場合
に比較して電力損失pBがほとんどの温度範囲で小さい
こともわかる。酸化第二スズ(5nO2)の添加量が0
.50重量%よシ小さいと添加しないものよシミ力損失
pBが大きくなり。As shown in Figure 1, when the frequency is 200 kHz, the temperature T at which the power loss pB reaches the minimum value when stannic oxide (5 nOz) is not added is about 60°C, whereas when the stannic oxide (5 nOz) It can be seen that as the amount of addition increases, the temperature at which the power loss pB is the minimum value shifts to the lower temperature side. Further, the amount of stannic oxide (SnO2) added is about 0.
It can also be seen that when the addition amount is 75% by weight, the power loss pB is smaller in most temperature ranges than in the case of other addition amounts (including 0 yen). Added amount of stannic oxide (5nO2) is 0
.. If the amount is smaller than 50% by weight, the staining force loss pB will be greater than that without addition.
又、酸化第二スズ(5n02 )の添加量が0.90重
量%を越えると添加しないものより電力損失pBが大き
くなる傾向にある。このことよ99周波数2O0kHz
においては、酸化第二スズを0.05〜0.90重量%
添加した方が、添加しないものよシ、特に低温側におい
て電力損失が小さくなることがわかる。Furthermore, when the amount of stannic oxide (5n02) added exceeds 0.90% by weight, the power loss pB tends to be larger than that without addition. This thing is 99 frequency 2O0kHz
In, 0.05 to 0.90% by weight of stannic oxide
It can be seen that when added, the power loss is smaller than when not added, especially on the low temperature side.
第2図に2本発明によシ得られた酸化物磁性材料AI(
副成分として0.018重量%の二酸化ケイ素(SiO
2) −0,045重量%の酸化カルシウム(CaO)
及び0.75重量%の酸化第二スズ(SnO2)を含有
)と、従来の酸化物磁性材料l62(副成分として0.
018重量%の二酸化ケイ素(SiO2)と0.045
重量%の酸化カルシウム(CaO)を含有し、酸化第二
スズ(5n02 )は添加しない)とA3(副成分とし
て0.010重量%の二酸化ケイ素(5i02 )と0
.030重量%の酸化カルシウム(Cab)を含有し、
酸化第二スズ(5n02 )は添加しない)の諸特性(
初透磁率μi、飽和磁束密度B86(磁化力150eに
おける磁束密度)CG)、残留磁束密度Br[G]、保
持力He(Oe〕及び比抵抗ρ〔Ω・帰〕)を示す。な
お主成分は、いずれも酸化第二鉄(ve2os )が5
2.5モル%、−酸化マンガン(MnO)が34.0モ
ル係及び酸化亜鉛(ZnO)が13.5 %ルチ含有し
ている。Figure 2 shows two oxide magnetic materials AI (
0.018% by weight of silicon dioxide (SiO
2) -0,045% by weight of calcium oxide (CaO)
and 0.75% by weight of stannic oxide (SnO2)), and the conventional oxide magnetic material l62 (containing 0.75% by weight of stannic oxide (SnO2)).
0.018 wt% silicon dioxide (SiO2) and 0.045
% by weight of calcium oxide (CaO) and no added stannic oxide (5n02)) and A3 (0.010% by weight of silicon dioxide (5i02) as accessory components).
.. Contains 030% by weight of calcium oxide (Cab),
Properties of (without adding stannic oxide (5n02))
Initial magnetic permeability μi, saturation magnetic flux density B86 (magnetic flux density at magnetizing force 150e) CG), residual magnetic flux density Br [G], coercive force He (Oe], and specific resistance ρ [Ω·return]) are shown. The main component in both cases is ferric oxide (ve2os).
It contains 2.5 mol %, 34.0 mol % of manganese oxide (MnO) and 13.5 mol % of zinc oxide (ZnO).
第2図よシ明らかな如く0本発明のもの屋1は。As is clear from FIG.
スイッチング電源用磁芯材料として求められる諸特性1
例えば初透磁率μiが約2500.飽和磁束密度B15
が約5000G及び残留磁束密度Brが1000G以下
という特性を十分に満たし、比抵抗ρも従来のものA2
及び屋3に比べて大幅に向上している。Characteristics required for magnetic core materials for switching power supplies 1
For example, the initial magnetic permeability μi is about 2500. Saturation magnetic flux density B15
satisfies the characteristics of approximately 5000G and residual magnetic flux density Br of 1000G or less, and the specific resistance ρ is also lower than that of the conventional A2
This is a significant improvement compared to 3.
以上のことより、添加物酸化第二スズ(Sn02)は、
スイッチング電源用磁芯材料として求められる諸特性を
十分に満たすと共に1周波数が2O0kHz以上の高周
波において、電力損失P B (kW/m3)を1例え
ば約0.75重量%の酸化第二スズ(SnO2)を添加
した場合、添加しない場合に比較して特に低い温度側(
例えば60℃以下)で約25%改善できることがわかる
。From the above, the additive tin oxide (Sn02) is
It sufficiently satisfies various properties required as a magnetic core material for switching power supplies, and also reduces power loss P B (kW/m3) at high frequencies of 2O0kHz or higher.For example, about 0.75% by weight of tin oxide (SnO2 ) is added, the temperature side is particularly lower (
For example, it can be seen that an improvement of about 25% can be achieved at temperatures below 60°C.
以上の説明で明らかなように、0.50−0.90重量
%の酸化第二スズ(SnO2)を添加することによシ、
スイッチング電源用材料として求められる諸特性を十分
に満足するとともに1周波数が2O0kHz以上の高周
波において従来のものよシミ力損失を低減できる低損失
酸化物磁性材料を提供でき。As is clear from the above explanation, by adding 0.50-0.90% by weight of stannic oxide (SnO2),
It is possible to provide a low-loss oxide magnetic material that fully satisfies various characteristics required as a material for a switching power supply and can reduce stain force loss compared to conventional materials at high frequencies of 200 kHz or higher.
高周波用磁芯材料として好適であシ、変圧器の小型化−
軽量化を計ることができる。Suitable as a magnetic core material for high frequency, miniaturization of transformers.
Weight reduction can be measured.
第1図は酸化第二スズ(5n02 )の添加量を・母う
メータとしたときの温度と電力損失の関係を示した図、
第2図は本発明及び従来の酸化物磁性材料の諸特性を示
した図である。
第1図
TEMP(’C)Figure 1 is a diagram showing the relationship between temperature and power loss when the amount of stannic oxide (5n02) added is used as the main meter.
FIG. 2 is a diagram showing various characteristics of the present invention and conventional oxide magnetic materials. Figure 1 TEMP('C)
Claims (1)
MnO)、10〜15モル%の酸化亜鉛(ZnO)及び
残部酸化第二鉄(Fe_2O_3)を含み、副成分とし
て0.04〜0.10重量%の酸化カルシウム(CaO
)と0.015〜0.100重量%の二酸化ケイ素(S
iO_2)を含む低損失酸化物磁性材料において、0.
50〜0.90重量%の酸化第二スズ(SnO_2)を
添加したことを特徴とする低損失酸化物磁性材料。1. 30 to 37 mol% manganese monoxide as the main component (
MnO), 10-15 mol% zinc oxide (ZnO) and the balance ferric oxide (Fe_2O_3), and 0.04-0.10 wt% calcium oxide (CaO) as an accessory component.
) and 0.015 to 0.100% by weight of silicon dioxide (S
iO_2) in a low-loss oxide magnetic material containing 0.
A low-loss oxide magnetic material characterized by adding 50 to 0.90% by weight of stannic oxide (SnO_2).
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP60092205A JPS61252609A (en) | 1985-05-01 | 1985-05-01 | Magnetic material of low-loss oxide |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP60092205A JPS61252609A (en) | 1985-05-01 | 1985-05-01 | Magnetic material of low-loss oxide |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS61252609A true JPS61252609A (en) | 1986-11-10 |
Family
ID=14047942
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP60092205A Pending JPS61252609A (en) | 1985-05-01 | 1985-05-01 | Magnetic material of low-loss oxide |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61252609A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS63281207A (en) * | 1987-05-14 | 1988-11-17 | Matsushita Electric Ind Co Ltd | Single crystal ferrite |
JPH0254902A (en) * | 1988-08-19 | 1990-02-23 | Sony Corp | Low-loss ferrite |
US6627103B2 (en) | 2000-03-31 | 2003-09-30 | Tdk Corporation | Mn-Zn ferrite production process, Mn-Zn ferrite, and ferrite core for power supplies |
-
1985
- 1985-05-01 JP JP60092205A patent/JPS61252609A/en active Pending
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS63281207A (en) * | 1987-05-14 | 1988-11-17 | Matsushita Electric Ind Co Ltd | Single crystal ferrite |
JPH0254902A (en) * | 1988-08-19 | 1990-02-23 | Sony Corp | Low-loss ferrite |
US6627103B2 (en) | 2000-03-31 | 2003-09-30 | Tdk Corporation | Mn-Zn ferrite production process, Mn-Zn ferrite, and ferrite core for power supplies |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
JPS61252609A (en) | Magnetic material of low-loss oxide | |
JPH081844B2 (en) | High frequency low loss ferrite for power supply | |
JPS61252606A (en) | Magnetic material of low-loss oxide | |
JPS58114401A (en) | Superlow loss ferrite for power source | |
JPH11238617A (en) | Manganese-zinc based ferrite | |
JPS61252611A (en) | Magnetic material of low-loss oxide | |
JP2001006916A (en) | Low loss oxide magnetic material | |
JPS61252607A (en) | Magnetic material of low-loss oxide | |
JPS61252610A (en) | Magnetic material of low-loss oxide | |
JPH0457628B2 (en) | ||
JP2627654B2 (en) | Low loss oxide magnetic material | |
JP2640479B2 (en) | Low loss oxide magnetic material | |
JPH03163804A (en) | Low loss oxide magnetic substance | |
JPS61252608A (en) | Magnetic material of low-loss oxide | |
JPH0124746B2 (en) | ||
JP2000269017A (en) | Oxide magnetic material | |
JP2541814B2 (en) | Low loss oxide magnetic material for power supply | |
JPH07130527A (en) | Oxide magnetic material | |
JP2627639B2 (en) | Low loss oxide magnetic material | |
JP3203494B2 (en) | Low loss oxide magnetic material | |
JPH01259509A (en) | Low loss oxide magnetic material | |
JPH01143307A (en) | Low-loss oxide magnetic material | |
JPH02284404A (en) | Low-loss oxide magnetic material | |
JP2003257724A (en) | Mn-Zn-BASED FERRITE | |
JPS6119086B2 (en) |