JPS5963705A - Transformer core - Google Patents
Transformer coreInfo
- Publication number
- JPS5963705A JPS5963705A JP57170549A JP17054982A JPS5963705A JP S5963705 A JPS5963705 A JP S5963705A JP 57170549 A JP57170549 A JP 57170549A JP 17054982 A JP17054982 A JP 17054982A JP S5963705 A JPS5963705 A JP S5963705A
- Authority
- JP
- Japan
- Prior art keywords
- loss
- porosity
- transformer
- transformer core
- lance
- 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
Links
- 239000000654 additive Substances 0.000 claims abstract description 3
- 239000000203 mixture Substances 0.000 claims abstract description 3
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 claims abstract 3
- 229910052681 coesite Inorganic materials 0.000 claims abstract 2
- 229910052906 cristobalite Inorganic materials 0.000 claims abstract 2
- 229910052682 stishovite Inorganic materials 0.000 claims abstract 2
- 229910052905 tridymite Inorganic materials 0.000 claims abstract 2
- 229910000859 α-Fe Inorganic materials 0.000 abstract description 4
- 230000000996 additive effect Effects 0.000 abstract 1
- JEIPFZHSYJVQDO-UHFFFAOYSA-N iron(III) oxide Inorganic materials O=[Fe]O[Fe]=O JEIPFZHSYJVQDO-UHFFFAOYSA-N 0.000 abstract 1
- 239000000377 silicon dioxide Substances 0.000 abstract 1
- 235000012239 silicon dioxide Nutrition 0.000 abstract 1
- 230000035699 permeability Effects 0.000 description 5
- 238000004519 manufacturing process Methods 0.000 description 2
- VZSRBBMJRBPUNF-UHFFFAOYSA-N 2-(2,3-dihydro-1H-inden-2-ylamino)-N-[3-oxo-3-(2,4,6,7-tetrahydrotriazolo[4,5-c]pyridin-5-yl)propyl]pyrimidine-5-carboxamide Chemical compound C1C(CC2=CC=CC=C12)NC1=NC=C(C=N1)C(=O)NCCC(N1CC2=C(CC1)NN=N2)=O VZSRBBMJRBPUNF-UHFFFAOYSA-N 0.000 description 1
- 241000023849 Coreura Species 0.000 description 1
- 241000406668 Loxodonta cyclotis Species 0.000 description 1
- 241000220218 Manilkara Species 0.000 description 1
- 230000006835 compression Effects 0.000 description 1
- 238000007906 compression Methods 0.000 description 1
- 239000013078 crystal Substances 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 238000010304 firing Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 239000000843 powder Substances 0.000 description 1
- 239000013589 supplement Substances 0.000 description 1
- 230000002747 voluntary effect Effects 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F1/00—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
- H01F1/01—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
- H01F1/03—Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
- H01F1/12—Magnets 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
- H01F1/34—Magnets 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
- H01F1/342—Oxides
- H01F1/344—Ferrites, 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)
- Compounds Of Iron (AREA)
- Magnetic Ceramics (AREA)
- Soft Magnetic Materials (AREA)
Abstract
Description
【発明の詳細な説明】
本fテ明は、焼結体の空孔率を3.5%以下と少なくし
た低損失1−ランスコノノに関づるものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a low-loss 1-lance powder in which the porosity of the sintered body is reduced to 3.5% or less.
一般に1ヘランス]アとしては、Mn−2n系の71ン
イi−が主に用いられている1、その際コアに要求され
る特性は、電磁気的損失の低減ぐあり、特に近江著しく
伸長してりるスイッチング電源用トランスコアは、高周
波化の点にJ3い−(五′iJますT:+ 77損失の
低減が重危と【トつてぎCいる。。In general, Mn-2n type 71-i-i- is mainly used as a material for the core.The characteristics required for the core in this case are reduction of electromagnetic loss, and in particular, Transformer cores for switching power supplies have high frequencies, and reduction of loss is a critical issue.
一般にトランスコアの損失は渦電流損失、ヒステリシス
損失、残留損失の和ぐ決定される。、これら損失Jnに
中で渦電流損失は、主に添加物、例えばca 、v、s
i等を加えることににリー電気抵抗を高めることで低減
が削られている1、また第2項のヒステリシス損失は、
焼成体の空孔率、結晶粒径、異相の45無等にJ、り変
化することが知られ(いる。したがって、ヒステリシス
損失の低減には主にての製造方法を考慮し作成すること
が重要どなっCくる。Generally, transformer core loss is determined by the sum of eddy current loss, hysteresis loss, and residual loss. , among these losses Jn, eddy current losses are mainly caused by additives, such as ca, v, s
The reduction is reduced by increasing the Lee electrical resistance in addition to adding i, etc., and the hysteresis loss in the second term is
It is known that the porosity, crystal grain size, and different phases of the fired body vary depending on the J value. Therefore, in order to reduce hysteresis loss, it is necessary to take into consideration the manufacturing method. It's important.
そこC本発明は、Mn−Zn系フェライトにおい(、そ
の製造方法を考慮し空孔率を少なくづ゛ることにj、す
、ヒステリシス損失を小さくり−ることで−17の損失
の低減化を割ったものである。Therefore, the present invention aims to reduce the porosity of Mn-Zn ferrite (by taking into consideration its manufacturing method), and by reducing the hysteresis loss. is divided by .
ここぐM++”Zn系フェライトにおいて、焼成体の空
孔率を小ならしめることにより加]−性あるいは耐摩耗
す11を改良したものに、例えば磁気ヘッド祠お1があ
る。しかしながら空孔率と高周波ぐの損失の関係は明確
化されていない。ざらに本発明のトランス−1アと大幅
に異なる点として、透磁率の第2次ピーク温度が上げら
れる。磁気l\ツド祠はそのピーク温度が室温イ1近で
あるのに対し、1・ランスコノノCはトランスの動作温
度(約80°C) (:Jシ1にでのピーク温度を設定
しくいること(−ある。For example, in the M++ Zn-based ferrite, there is a magnetic head mill 1 which improves the addi- tivity or wear resistance by reducing the porosity of the fired body.However, the porosity and The relationship between loss at high frequencies has not been clarified.Roughly speaking, the major difference from the transformer 1 of the present invention is that the secondary peak temperature of magnetic permeability is raised. While the room temperature is close to 1, the operating temperature of the transformer (approximately 80°C) is approximately 80°C.
これは〜般に透磁率の第2次ピーク渇度イ」近ぐ」〕′
の損失が最小となることによるぜ:)の(・ある。さら
に磁気ヘッド刊には、高周波で・の仏号を記録。This is generally close to the second peak of magnetic permeability.'
This is due to the fact that the loss of is minimized: )'s (・There is.Furthermore, the magnetic head edition records the Buddhist name of ・ at high frequency.
再生りることが必要Cあるため、高周波で高い透磁率を
要求される。これに対し本発明の1−ランス] 77は
イれ稈高い透磁率必要なく、例λば0.1へ48 Z
′C−1500〜2500程度(パある。したが・ンて
上記の様/’c諸特↑j1の違いから当然のことイzが
ら両晋の組成領域は異4rるものである。Because it needs to be regenerated, high magnetic permeability is required at high frequencies. On the other hand, the 1-lance of the present invention] 77 does not require high magnetic permeability, for example, λ to 0.1 48 Z
'C-1,500 to 2,500 (there are some, but as mentioned above, the composition ranges of the two countries are of course different from each other due to the differences in the various characteristics ↑j1).
jス下に本発明を実施例により訂細に説明りる。The present invention will be explained in detail below using examples.
実施例1
1 (: 2 Q 3 : 53.5’[ル%、 M
n O: 36.01.ル%。Example 1 1 (: 2 Q 3 : 53.5'[%, M
nO: 36.01. le%.
/ n Q : 10.5七ル%およびCaOを0.1
wt%となる様に、Fa 203 、Mn O,Zn
O,Ca CO3を秤岨し混合した。その後700〜1
200℃で仮焼成し、微粉砕し圧縮成形後1300〜1
450℃C・焼成した。/nQ: 10.5% and 0.1% CaO
Fa203, MnO, Zn so that wt%
O, Ca and CO3 were weighed and mixed. After that 700-1
Pre-calcined at 200℃, finely pulverized and compression molded to 1300~1
It was fired at 450°C.
1!1られた焼成体試料の緒特性測定結果を第1表に承
り。Table 1 shows the results of measuring the properties of the fired body samples.
第1表
以−1の実施例より明らかなごとく、本発明のトランス
1アは空孔率を減少さヒることにより、損失を減少さけ
ることができる。また3、5%以十Cある場合、1−ラ
ンス−」アの損失を減少されないため空孔率は:3.5
%以干にり−ることが理想的である。As is clear from the examples shown in Table 1-1, the transformer 1a of the present invention can reduce loss by reducing the porosity. In addition, when there is more than 3.5% of C, the loss of 1-lance-'a is not reduced, so the porosity is: 3.5
Ideally, it should be more than %.
実施例2
[0203: 52.5モル%、 M ++ Q :
37.0’Eル%。Example 2 [0203: 52.5 mol%, M ++ Q:
37.0'Ele%.
Z ++ O: 10.5モル%およびCaOをg、i
wt%となる桶に、実施例1と同様の方法で試別を作成
しlこ、。Z ++ O: 10.5 mol% and CaO g, i
A sample was prepared in the same manner as in Example 1 in a bucket containing wt%.
11?られた試料の緒特性を第2表に示す。11? Table 2 shows the properties of the samples obtained.
第2表
以上の実施例Jこり明らかなごとく、実施例1と同様、
空孔率を減少さIることにJ:す1〜ランス−1jνの
損失が減少していることが判る。As is clear from Example J in Table 2 and above, similar to Example 1,
It can be seen that by decreasing the porosity, the loss of J:su1 to lance-1jv is reduced.
実施例3
1Te 203 : 53.5モル%、 Mll O
: 34,5モル%。Example 3 1Te203: 53.5 mol%, MllO
: 34.5 mol%.
l n O: 12.0−Eル%およびCaOをO,1
wt%となる様に、実施例1ど同様の方法で試料を作成
し緒特性を測定した。測定結果を第3表に示づ。lnO: 12.0-El% and CaO to O,1
Samples were prepared in the same manner as in Example 1, and their properties were measured so as to achieve the same wt%. The measurement results are shown in Table 3.
第3表
以上の様に実施例1と同様空孔率を減少させることによ
り、トランスコアのj置火が減少しCいることがわかる
。As shown in Table 3 and above, it can be seen that by reducing the porosity as in Example 1, the J firing of the transformer core is reduced.
実施例4
先に実施例1により得られたAおよびCの試#1につい
(、周波数に対づるトランス」アの損失値(〒渇)を測
定した。この結果を第1図に示覆。Example 4 For test #1 of A and C obtained earlier in Example 1, the loss value (loss) of transformer A versus frequency was measured. The results are shown in FIG.
図から縦軸の切片がヒステリシス損失に相当りるか、そ
の値を換nするど、試料Aが約!i70 mw/C11
13の損失値に対し、空孔率を減少さぽた試着ICぐは
約280 mw/cm”と非常に小さな偵となることが
わかる。From the figure, we can find out whether the intercept on the vertical axis corresponds to the hysteresis loss or not, by converting the value to n. i70 mw/C11
It can be seen that compared to the loss value of 13, the decrease in the porosity of the Sapota try-on IC results in a very small loss of about 280 mw/cm.
さらに両試斜単体での温度上昇を測定した結果を第2図
に示す。図から明らかなごとく、空孔率を減少さlた試
別Cは、試料Δに比しi〜ランスニ1アの温度上Piを
極力低下さけることがCきる。Furthermore, Figure 2 shows the results of measuring the temperature rise in both test slopes. As is clear from the figure, sample C with reduced porosity can avoid lowering the temperature Pi of i to lance nia 1 as much as possible compared to sample Δ.
以上実施例1〜4に述べた様に、Mll −Z n系ノ
1ライ1−を1−ランスコアとして用いる場合、焼成体
の空孔率を3.5%以上にJることによって低損失1−
ランスコアを得ることがCきる。As described above in Examples 1 to 4, when Mll-Z n-based No. 1 Lie 1- is used as a 1-lance core, low loss can be achieved by setting the porosity of the fired body to 3.5% or more. 1-
You can get a run score.
第1図は!・ランスコアの損失の周波歓待↑z1を示し
、第2図は1〜ランスニ一1ア単体ぐの温度上胃埴を示
り図(゛ある。
(ZHfi幻/xlf ) 堵昇’g/、7dQ(l
ap) 118=し7g<t/z−$f;tr:→
(ζC(手続補正書(自発)
11ii 1+’681i21^411111゛1の表
示
昭f、1157 ?l”1.旨′I願第170549
′/;発 明 の とl 称 トランスコア浦1
1をすると
R+1・50B1 l’l +”/合属株式会社代J
) M ’、u■9!) 1l
li、 、)、代 f甲 人
i、・: 所 東μ;一部り代111区丸の1ノ
・ダ1゛10計2シ;ll+’/箔属t1、式会と1内
電話 東京 284−4642補市の月象
明細書の「発明の詳細な説明」の欄。
補iEの内容
1、 明細書の「発明の詳細な説明」の欄の記載全下記
の通り訂正する。
記
(1)明細書第2頁第1行の「損失項に」を「損失項の
」に訂正する。
(2)同書第3頁第8行の「透磁率」の後だ「け」を挿
入する。
(3)同書第4頁第10行の「損失を」全「損失は」に
訂正する。
以 上Figure 1 is!・The frequency reception ↑z1 of the loss of the Lance score is shown, and Figure 2 shows the temperature of the temperature of the 1~Lance 11A single unit. 7dQ(l
ap) 118=shi7g<t/z−$f;tr:→
(ζC (procedural amendment (voluntary) 11ii 1+'681i21^411111゛1 indication Showf, 1157?l"1. Purport'I Application No. 170549
'/; name of the invention Trans Core Ura 1
If you do 1, you get R+1・50B1 l'l +”/Josei Co., Ltd. J
) M', u■9! ) 1l
li, ,), day fko person i,...: place east μ; part charge 111 ku maru no 1 no da 1゛10 total 2 shi; ll+'/haku t1, ceremony and 1 phone Tokyo 284-4642 ``Detailed Description of the Invention'' column of the Lunar Elephant Specification by Hoichi. Contents of Supplement iE 1: All statements in the "Detailed Description of the Invention" column of the specification are corrected as follows. (1) In the first line of page 2 of the specification, "in the loss term" is corrected to "of the loss term." (2) Insert "ke" after "magnetic permeability" on page 3, line 8 of the same book. (3) On page 4, line 10 of the same book, "loss wo" is corrected to "loss wa."that's all
Claims (1)
32−40. Z n O:8〜13七ル%の組成物
に、かつ所望(こよりCa O。 V2’Os 、Si 02等の添加物を加えたトランス
IT]Mn−7nフ1ライI−におご1で、その焼結体
の空孔率を3.j)%以下にすることを特徴とする低損
失1〜シンスコア。[Claims] lc 203: to 48! 16. M II O:
32-40. ZnO: 8 to 13% of the composition, and the desired (trans IT with additives such as CaO, V2'Os, Si02, etc.) Mn-7n fly I-. and a low loss 1 to thin core, characterized in that the porosity of the sintered body is 3.j)% or less.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP57170549A JPS5963705A (en) | 1982-09-29 | 1982-09-29 | Transformer core |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP57170549A JPS5963705A (en) | 1982-09-29 | 1982-09-29 | Transformer core |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS5963705A true JPS5963705A (en) | 1984-04-11 |
JPS6119086B2 JPS6119086B2 (en) | 1986-05-15 |
Family
ID=15906935
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP57170549A Granted JPS5963705A (en) | 1982-09-29 | 1982-09-29 | Transformer core |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5963705A (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS63116406A (en) * | 1986-11-05 | 1988-05-20 | Tdk Corp | Ferrite core |
JPH01136309A (en) * | 1987-11-24 | 1989-05-29 | Mitsubishi Electric Corp | Low loss oxide magnetic material |
US4863625A (en) * | 1984-10-30 | 1989-09-05 | U.S. Philips Corporation | Titanium-containing and cobalt-containing manganese-zinc ferrite core and method of manufacturing same |
JP2005272229A (en) * | 2004-03-25 | 2005-10-06 | Jfe Ferrite Corp | HIGH SATURATION MAGNETIC FLUX DENSITY Mn-Zn-Ni-BASED FERRITE |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5328633A (en) * | 1976-08-28 | 1978-03-17 | Yamasan Shiyouji Kk | Decoration material for building |
JPS5836974A (en) * | 1981-08-27 | 1983-03-04 | 住友特殊金属株式会社 | Low magnetic loss mn-zn ferrite and manufacture |
-
1982
- 1982-09-29 JP JP57170549A patent/JPS5963705A/en active Granted
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5328633A (en) * | 1976-08-28 | 1978-03-17 | Yamasan Shiyouji Kk | Decoration material for building |
JPS5836974A (en) * | 1981-08-27 | 1983-03-04 | 住友特殊金属株式会社 | Low magnetic loss mn-zn ferrite and manufacture |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4863625A (en) * | 1984-10-30 | 1989-09-05 | U.S. Philips Corporation | Titanium-containing and cobalt-containing manganese-zinc ferrite core and method of manufacturing same |
JPS63116406A (en) * | 1986-11-05 | 1988-05-20 | Tdk Corp | Ferrite core |
JPH01136309A (en) * | 1987-11-24 | 1989-05-29 | Mitsubishi Electric Corp | Low loss oxide magnetic material |
JP2005272229A (en) * | 2004-03-25 | 2005-10-06 | Jfe Ferrite Corp | HIGH SATURATION MAGNETIC FLUX DENSITY Mn-Zn-Ni-BASED FERRITE |
Also Published As
Publication number | Publication date |
---|---|
JPS6119086B2 (en) | 1986-05-15 |
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