JPH07257966A - Ni-containing low loss ferrite for power source - Google Patents
Ni-containing low loss ferrite for power sourceInfo
- Publication number
- JPH07257966A JPH07257966A JP6072498A JP7249894A JPH07257966A JP H07257966 A JPH07257966 A JP H07257966A JP 6072498 A JP6072498 A JP 6072498A JP 7249894 A JP7249894 A JP 7249894A JP H07257966 A JPH07257966 A JP H07257966A
- Authority
- JP
- Japan
- Prior art keywords
- loss
- ferrite
- less
- core
- mol
- 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
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は、スイッチング電源、液
晶バックライト等のトランスに用いられるフェライト材
料に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a ferrite material used for transformers such as switching power supplies and liquid crystal backlights.
【0002】[0002]
【従来の技術】スイッチング電源、液晶バックライト
は、民生機器をはじめOA、産業用機器へと幅広い利用
が進んでおり、現在、小型、薄型、軽量化が図られてい
る。このスイッチング電源や液晶バックライト等に使用
されるトランスには、従来、Mn系のフェライトコアが
使用されていた。2. Description of the Related Art Switching power supplies and liquid crystal backlights have been widely used in consumer equipment, office automation equipment, and industrial equipment, and are currently being made smaller, thinner, and lighter. Conventionally, a Mn-based ferrite core has been used for the transformer used for the switching power supply, the liquid crystal backlight, and the like.
【0003】[0003]
【発明が解決しようとする課題】Mn系のフェライトコ
アは、飽和磁束密度、透磁率が大きく、また損失(コア
ロス)が10kW/m3程度(50kHz、50mT)
と小さいという特長があり、これまでスイッチング電源
や液晶バックライト等のトランスに用いられてきた。し
かしながら、抵抗率が10Ω・m程度と比較的低く、コ
アに直接巻線をすると漏れ電流が発生する。このため、
スイッチング電源等のトランスとしては、Mn系のフェ
ライトコアを使用する場合、コアにボビンをかぶせた
り、絶縁被膜等の処理を行ってから巻線を行っており、
製造コストが高く、小型化が難しいという問題があっ
た。これに対し、Ni系のフェライトコアは、抵抗率が
106Ω・m程度と非常に高く、コアに直接巻線をする
ことが可能であるが、損失(コアロス)が60kW/m
3(50kHz、50mT)程度と大きため、コアが発
熱し易く、スイッチング電源等のトランスとして適して
いなかった。本発明は、上記のことを鑑みて、抵抗率の
高いNi系フェライトにて、損失(コアロス)が小さ
く、スイッチング電源等のトランスとして使用できるフ
ェライト材料を提供することを目的とする。The Mn-based ferrite core has a large saturation magnetic flux density and permeability, and a loss (core loss) of about 10 kW / m 3 (50 kHz, 50 mT).
It has been used for transformers such as switching power supplies and liquid crystal backlights. However, the resistivity is relatively low, about 10 Ω · m, and leakage current occurs when the core is directly wound. For this reason,
When a Mn-based ferrite core is used as a transformer for a switching power supply or the like, the core is covered with a bobbin or treated with an insulating film or the like before winding.
There is a problem that the manufacturing cost is high and miniaturization is difficult. On the other hand, the Ni-based ferrite core has a very high resistivity of about 10 6 Ω · m and can be wound directly on the core, but the loss (core loss) is 60 kW / m.
Since it is as large as about 3 (50 kHz, 50 mT), the core easily generates heat and is not suitable for a transformer such as a switching power supply. In view of the above, an object of the present invention is to provide a ferrite material having a high resistivity and a small loss (core loss), which can be used as a transformer for a switching power supply or the like.
【0004】[0004]
【課題を解決するための手段】本発明は、上記問題点を
解決するために、Fe2O3 40〜52.5mol%、
NiO 5〜47.5mol%、ZnO 35mol%
以下から成る組成を主成分とするフェライトであって、
焼結体中のPの含有量を66ppm未満とし、かつ焼成
密度が5.1×103kg/m3以上、結晶粒径が10μ
m以下とするものである。本発明において、フェライト
材料の組成範囲を限定した理由は、以下の通りである。
主成分の内、Fe2O3が52.5mol%を越える
時、あるいはNiOが5mol%未満の時、抵抗率が低
く、コアに直接巻線をすることができない。ZnOが3
5mol%を越える時、キュリー温度が100℃以下と
なり、実用的でない。よって、請求範囲に示す主成分組
成が限定される。また、焼成密度が5.1×103kg
/m3未満となるか、あるいは結晶粒径が10μmを越
えると、損失(コアロス)が大きくなる。なお、本発明
のフェライト材料は、前記の組成を有するものであれ
ば、製造方法には、特に制限はない。SUMMARY OF THE INVENTION In order to solve the above problems, the present invention provides Fe 2 O 3 of 40 to 52.5 mol%,
NiO 5-47.5 mol%, ZnO 35 mol%
A ferrite containing the following composition as a main component,
The content of P in the sintered body is less than 66 ppm, the firing density is 5.1 × 10 3 kg / m 3 or more, and the grain size is 10 μm.
m or less. In the present invention, the reason why the composition range of the ferrite material is limited is as follows.
When Fe2O3 exceeds 52.5 mol% or NiO is less than 5 mol% among the main components, the resistivity is low and the core cannot be directly wound. ZnO is 3
When it exceeds 5 mol%, the Curie temperature becomes 100 ° C. or lower, which is not practical. Therefore, the main component composition shown in the claims is limited. Moreover, the firing density is 5.1 × 10 3 kg.
If it is less than / m 3 or the crystal grain size exceeds 10 μm, the loss (core loss) increases. The ferrite material of the present invention is not particularly limited in its production method as long as it has the above composition.
【0005】[0005]
【作用】従来のNi系フェライト材料では、上述の如
く、損失(コアロス)が60kW/m3(50kHz、
50mT)と大きく、スイッチング電源等のトランスと
して適さなかった。本発明は、Ni系フェライト材料
で、スイッチング電源等のトランスとして使用できる材
料を研究した所、Pの含有量が多いと、焼結体の結晶組
織中にPの偏析を生じ、このPの偏析を生じると損失
(コアロス)が大きくなることを見い出し、焼結体中の
Pの含有量が66ppm未満であると焼結体の結晶組織
中のPの偏析が抑制され、低損失となるものであり、こ
のとき焼成密度が5.1×103kg/m3以上、結晶粒
径が10μm以下のとき、損失(コアロス)が30kW
/m3以下(50kHz、50mT)と低損失で、スイ
ッチング電源等のトランスとして使用できるフェライト
材料が得られる。With the conventional Ni-based ferrite material, as described above, the loss (core loss) is 60 kW / m 3 (50 kHz,
It was as large as 50 mT) and was not suitable for a transformer such as a switching power supply. In the present invention, as a result of researching a Ni-based ferrite material that can be used as a transformer for a switching power supply or the like, when the content of P is large, P is segregated in the crystal structure of the sintered body, and this P segregation occurs. It has been found that the loss (core loss) increases when the occurrence of the above occurs, and when the content of P in the sintered body is less than 66 ppm, the segregation of P in the crystal structure of the sintered body is suppressed and the loss becomes low. When the firing density is 5.1 × 10 3 kg / m 3 or more and the crystal grain size is 10 μm or less, the loss (core loss) is 30 kW.
/ M 3 or less (50 kHz, 50 mT), a low loss, and a ferrite material that can be used as a transformer for a switching power supply or the like can be obtained.
【0006】[0006]
【実施例】以下に、本発明に係るフェライト材料の実施
例を詳細に説明する。Pの含有量が10ppm以下のF
e2O3 49.45mol%、ZnO 29.75mo
l%、NiO 14.80mol%およびCuO 6.
00mol%相当量の素原料粉末を秤量し、これに所定
量のイオン交換水を添加したものをボールミルにて4時
間混合し、電気炉を用いて最高温度850℃で1.5時
間仮焼した後、これを炉冷し、40メッシュのふるいで
解砕する。しかる後、再び所定量のイオン交換水を添加
したものをボールミルにて6時間粉砕し、粉砕されたス
ラリー状の原料を乾燥および解砕する。これにバインダ
ー(ポリビニルアルコール)を加えて造粒し、40メッ
シュのふるいにて整粒した顆粒を乾式圧縮成形機と金型
を用いて、外径16.8mm、内径8.5mm、高さ
5.4mmのリング状コアに成形圧1.5ton/cm
2で成形し、これを大気中、1100℃で1.5時間焼
成した。得られた各試料の焼成密度を測定した後、周波
数50kHz、磁束密度50mTの測定条件において2
0〜140℃の温度範囲で損失(コアロス)を測定し
た。結果を図1に示す。また、焼結体の結晶組織(結晶
粒径、組成分布)の観察を行った。この実施例によれ
ば、電源用フェライトとして十分に使用できる程度に、
損失(コアロス)の小さいNi系フェライトを得ること
ができた。また、結晶組織中にPの偏析はなかった。さ
らに主成分組成およびFe2O3以外の素原料を同一と
し、また試料の作製方法を同一手順として、Pの含有量
が異なる種々のFe2O3を使って試料を作製し、上記実
施例と同じ条件で焼成密度、損失(コアロス)を測定
し、焼結体の結晶組織(結晶粒径、組成分布)の観察を
行った。結果を表1に示す。EXAMPLES Examples of the ferrite material according to the present invention will be described in detail below. F with a P content of 10 ppm or less
e 2 O 3 49.45 mol%, ZnO 29.75mo
1%, NiO 14.80 mol% and CuO 6.
A raw material powder in an amount equivalent to 00 mol% was weighed, a predetermined amount of ion-exchanged water was added thereto, and the mixture was mixed in a ball mill for 4 hours and calcined at a maximum temperature of 850 ° C. for 1.5 hours using an electric furnace. Then, this is cooled in an oven and crushed with a 40 mesh sieve. After that, a material to which a predetermined amount of ion-exchanged water has been added is pulverized by a ball mill for 6 hours, and the pulverized slurry raw material is dried and pulverized. A binder (polyvinyl alcohol) was added to this and granulated, and the granules sized with a 40-mesh sieve were used with a dry compression molding machine and a mold to have an outer diameter of 16.8 mm, an inner diameter of 8.5 mm, and a height of 5 Molding pressure of 1.5 ton / cm on a 4 mm ring-shaped core
Molded in 2 and fired in air at 1100 ° C. for 1.5 hours. After measuring the firing density of each of the obtained samples, 2 under the conditions of a frequency of 50 kHz and a magnetic flux density of 50 mT.
The loss (core loss) was measured in the temperature range of 0 to 140 ° C. The results are shown in Fig. 1. Further, the crystal structure (crystal grain size, composition distribution) of the sintered body was observed. According to this example, to the extent that it can be sufficiently used as a power ferrite,
It was possible to obtain a Ni-based ferrite with a small loss (core loss). Further, there was no segregation of P in the crystal structure. Further, using the same raw materials other than the main component composition and Fe 2 O 3 , and using the same sample preparation method, samples were prepared using various Fe 2 O 3 with different P contents. The firing density and loss (core loss) were measured under the same conditions as above, and the crystal structure (crystal grain size, composition distribution) of the sintered body was observed. The results are shown in Table 1.
【0007】[0007]
【表1】 [Table 1]
【0008】この表1からわかるとおり、焼結体中のP
の含有量が66ppm未満、焼成密度が5.1×103
kg/m3以上、及び結晶粒径が10μm以下の場合、
結晶組織中にPの偏析がなく、低損失(コアロスが30
kW/m3以下)なフェライトが得られた。なお、焼結
体中に含まれるPの含有量は、原料中のFe2O3量とF
e2O3素原料中のPの含有量から計算した。表1の実施
例3について、ICP(誘電結合プラズマ発光分光分析
法)により、焼結体中のPの含有量を分析した所、測定
値は45ppmとなり、前記、計算方法により求めた値
とほぼ一致した。次に、Pの含有量が10ppm以下の
Fe2O3 49.60mol%、ZnO32.80mo
l%およびNiO 17.60mol%相当量の素原料
粉末を秤量し、上記実施例と同一手順でリング状コアを
成形し、これを大気中、1200℃で1.5時間焼成し
た。得られた各試料の焼成密度、損失(コアロス)の測
定を、上記実施例と同じ条件で行った。また、焼結体の
結晶組織(結晶粒径、組成分布)の観察を行った。さら
に主成分組成およびFe2O3以外の素原料を同一とし、
また試料の作製方法を同一手順として、Pの含有量が異
なる種々のFe2O3を使って試料を作製し、上記実施例
と同じ条件で焼成密度、損失(コアロス)を測定し、焼
結体の結晶組織(結晶粒径、組成分布)の観察を行っ
た。結果を表2に示す。As can be seen from Table 1, P in the sintered body
Content of less than 66 ppm, firing density of 5.1 × 10 3
In the case of kg / m 3 or more and the crystal grain size is 10 μm or less,
There is no segregation of P in the crystal structure and low loss (core loss is 30
Ferrite of kW / m 3 or less) was obtained. In addition, the content of P contained in the sintered body is the amount of Fe 2 O 3 in the raw material and the content of F.
It was calculated from the content of P in the e 2 O 3 raw material. For Example 3 in Table 1, when the content of P in the sintered body was analyzed by ICP (Dielectric Coupling Plasma Atomic Emission Spectroscopy), the measured value was 45 ppm, which was almost the same as the value obtained by the above calculation method. Matched Next, P content of 10 ppm or less Fe 2 O 3 49.60 mol%, ZnO 32.80mo
1% and NiO 17.60 mol% equivalent raw material powders were weighed, a ring-shaped core was formed by the same procedure as in the above-mentioned example, and this was fired at 1200 ° C. for 1.5 hours in the atmosphere. The firing density and the loss (core loss) of each of the obtained samples were measured under the same conditions as in the above-mentioned examples. Further, the crystal structure (crystal grain size, composition distribution) of the sintered body was observed. Furthermore, the raw materials other than the main component composition and Fe 2 O 3 are the same,
Also, using the same procedure as the sample preparation method, samples were prepared using various Fe 2 O 3 having different P contents, and the firing density and loss (core loss) were measured under the same conditions as those in the above-mentioned examples, and sintering was performed. The crystal structure of the body (crystal grain size, composition distribution) was observed. The results are shown in Table 2.
【0009】[0009]
【表2】 [Table 2]
【0010】この表2からわかるとおり、焼結体中のP
の含有量が66ppm未満、焼成密度が5.1×103
kg/m3以上、及び結晶粒径が10μm以下の場合、
結晶組織中にPの偏析がなく、低損失(コアロスが30
kW/m3以下)なフェライトが得られた。なお、他の
Ni系フェライト(Ni―Mg―Cu―Znフェライ
ト、Ni―Mg―Znフェライト)についても、上記と
同様の検討を行った所、焼結体中のPの含有量を66p
pm未満、焼成密度が5.1×103kg/m3以上、及
び結晶粒径が10μm以下に抑えることにより、損失
(コアロス)が大幅に改善された。As can be seen from Table 2, P in the sintered body
Content of less than 66 ppm, firing density of 5.1 × 10 3
In the case of kg / m 3 or more and the crystal grain size is 10 μm or less,
There is no segregation of P in the crystal structure and low loss (core loss is 30
Ferrite of kW / m 3 or less) was obtained. In addition, the same examination as above was performed for other Ni-based ferrites (Ni-Mg-Cu-Zn ferrite, Ni-Mg-Zn ferrite), and it was found that the P content in the sintered body was 66p.
The loss (core loss) was significantly improved by suppressing the calcination density to less than pm, the firing density to 5.1 × 10 3 kg / m 3 or more, and the crystal grain size to 10 μm or less.
【0011】[0011]
【発明の効果】Ni系フェライト材料において、焼結体
中のPの含有量を66ppm未満、焼成密度を5.1×
103kg/m3以上、及び結晶粒径が10μm以下に抑
えることにより、損失(コアロス)が小さく、抵抗率の
高いフェライト材料が得られ、スイッチング電源等のト
ランス用として有用であり、トランスの製造コストの低
減、小型化が可能になる。EFFECT OF THE INVENTION In the Ni-based ferrite material, the content of P in the sintered body is less than 66 ppm and the firing density is 5.1 ×.
By controlling the crystal grain size to 10 3 kg / m 3 or more and the crystal grain size to 10 μm or less, a ferrite material having a small loss (core loss) and a high resistivity can be obtained, which is useful for a transformer such as a switching power supply. The manufacturing cost can be reduced and the size can be reduced.
【図1】本発明におけるNi系低損失磁性材料の損失
(コアロス)の温度特性を表す図である。FIG. 1 is a diagram showing temperature characteristics of loss (core loss) of a Ni-based low loss magnetic material according to the present invention.
Claims (1)
iO 5〜47.5mol%、ZnO 35mol%以
下から成る組成を主成分とし、焼結体中のPの含有量が
66ppm未満であり、かつ焼成密度が5.1×103
kg/m3以上で結晶粒径が10μm以下であることを
特徴とするNi系電源用低損失フェライト。1. Fe 2 O 3 40-52.5 mol%, N
The main component is a composition of 5 to 47.5 mol% of iO and 35 mol% or less of ZnO, the content of P in the sintered body is less than 66 ppm, and the firing density is 5.1 × 10 3.
A low-loss ferrite for Ni-based power supplies, which has a crystal grain size of 10 μm or less at kg / m 3 or more.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP6072498A JPH07257966A (en) | 1994-03-16 | 1994-03-16 | Ni-containing low loss ferrite for power source |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP6072498A JPH07257966A (en) | 1994-03-16 | 1994-03-16 | Ni-containing low loss ferrite for power source |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH07257966A true JPH07257966A (en) | 1995-10-09 |
Family
ID=13491063
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP6072498A Pending JPH07257966A (en) | 1994-03-16 | 1994-03-16 | Ni-containing low loss ferrite for power source |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH07257966A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US7524433B2 (en) * | 2004-05-21 | 2009-04-28 | Tdk Corporation | Ferrite material |
-
1994
- 1994-03-16 JP JP6072498A patent/JPH07257966A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US7524433B2 (en) * | 2004-05-21 | 2009-04-28 | Tdk Corporation | Ferrite material |
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