JPS59121806A - High-frequency magnetic material - Google Patents
High-frequency magnetic materialInfo
- Publication number
- JPS59121806A JPS59121806A JP57233369A JP23336982A JPS59121806A JP S59121806 A JPS59121806 A JP S59121806A JP 57233369 A JP57233369 A JP 57233369A JP 23336982 A JP23336982 A JP 23336982A JP S59121806 A JPS59121806 A JP S59121806A
- Authority
- JP
- Japan
- Prior art keywords
- temperature coefficient
- chemical formula
- negative
- density
- 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
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
Abstract
Description
【発明の詳細な説明】
本発明は高周波で用いられるフェライト磁心の温度係数
に関するものである。各種高周波回路のインダクタンス
素子は磁心としてのフェライトコアおよびボビンに巻回
されたコイルとより形成されている。このインダクタン
ス素子を使用した回路は特に、より高周波で動作するに
従い、周囲の温度変化に対して安定であることが重要で
ある。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a temperature coefficient of a ferrite magnetic core used at high frequencies. Inductance elements of various high frequency circuits are formed from a ferrite core serving as a magnetic core and a coil wound around a bobbin. Particularly as circuits using this inductance element operate at higher frequencies, it is important that they be stable against changes in ambient temperature.
温度変化に対して安定とするため従来採用されてきた手
段は以下である。すなわち通常コンデンサおよびインダ
クタンス素子の組み合せで回路が構成されているため、
両者を合せた温度係数が小さくなるように材質を選定す
るというものである。The following measures have been conventionally adopted to ensure stability against temperature changes. In other words, since the circuit is usually composed of a combination of capacitors and inductance elements,
The material is selected so that the combined temperature coefficient of both is small.
この選定は、一般にコンデンサの容量Gヨ負の濃度係数
をもつことから、これに対応して素子のインダクタンス
、言いかえればフェライト磁心の初透磁率の温度係数が
僅か正(通常20〜1ooxio’/deg )のもの
となることであった。しかしながらこの選定により得ら
れる回路全体の温度係数はフェライト磁心どコンデンサ
以外の他の部品、特にコルそのものの温度係数が正のた
め、充分満足出来るものどは言えない。この点をざらに
改善するためにはフェライト磁心の温度係数を負のもの
とすれば可能であるがこのような材料を得ることは困難
である。初透磁率の温度係数が負である材料どしては、
特願昭53−72567.72568があるが、これら
では密度が高々4.5 g/cm3にしか過ぎず製品強
度に難点があった。This selection is made because the capacitance G of the capacitor generally has a negative concentration coefficient. deg). However, it cannot be said that the temperature coefficient of the entire circuit obtained by this selection is fully satisfactory because the temperature coefficient of other parts other than the ferrite core and the capacitor, especially the coil itself, is positive. In order to roughly improve this point, it is possible to make the temperature coefficient of the ferrite magnetic core negative, but it is difficult to obtain such a material. Materials with a negative temperature coefficient of initial permeability are:
There is Japanese Patent Application No. 53-72567.72568, but these had a density of only 4.5 g/cm@3 at most and had a drawback in product strength.
本発明はこれにざらにV2O5を少量添加することによ
り、負の温度係数を維持しかつ密度の向上をはかるもの
である。The present invention aims to maintain a negative temperature coefficient and improve density by roughly adding a small amount of V2O5.
以下に実施例を述べ説明する。Examples will be described below.
実施例1
化学式でN’O−’l’l COo、2q 「1.qf
J o4 となるようにNi O,CO203,Fe2
O3を秤皐し、これに8! 2030.5wt%、 S
i 02 0.5wt%、V2O5を化学式表示で0.
01相当添加した粉体を水を媒体としてボールミル中に
て24時間混合した。Example 1 The chemical formula is N'O-'l'l COo, 2q "1.qf
NiO, CO203, Fe2 so that J o4
I weighed O3 and got 8! 2030.5wt%, S
i 02 0.5wt%, V2O5 in chemical formula 0.
The powder to which 0.01 was added was mixed for 24 hours in a ball mill using water as a medium.
該混合粉を大気中にて950°Cで仮焼の後同じくボー
ルミル中で24時間の湿式粉砕を施した。該粉砕粉をP
VA溶液を用い造粒の後リング状に成形した成形体を大
気中にて1100℃で3時間の焼成を行なった。この試
料の特性をV 205を添加しないものの結果と合せ第
1表に示す。The mixed powder was calcined at 950°C in the air and then wet-pulverized in a ball mill for 24 hours. The pulverized powder is P
After granulation using VA solution, the ring-shaped molded body was fired at 1100° C. for 3 hours in the atmosphere. The properties of this sample are shown in Table 1 along with the results without the addition of V205.
第1表 第1表で初透磁率の温度係数は次式で定義した。Table 1 In Table 1, the temperature coefficient of initial magnetic permeability is defined by the following formula.
この温度係数は0〜80℃の間で一様に負であった。This temperature coefficient was uniformly negative between 0 and 80°C.
実施例2
化学式でN i o、5 COo、o+5 F e 1
.’?404となる採索原料を秤吊し、これにBi 2
03 1.5wt%、3i020.3wt%、V2O5
を化学式相当r 0.03添加した混合物を実施例1と
同一の処理を施し、大気中1050℃で焼成したものの
特性を第2表に示す。この温度係数も0〜80℃で一様
な負の値で′あった。Example 2 Chemical formula: Nio, 5 COo, o+5 Fe 1
.. '? 404 was weighed and Bi 2 was added to it.
03 1.5wt%, 3i020.3wt%, V2O5
Table 2 shows the properties of a mixture in which 0.03 of R = 0.03 was added, which was subjected to the same treatment as in Example 1 and fired at 1050° C. in the atmosphere. This temperature coefficient was also a uniform negative value from 0 to 80°C.
第2表
これら実施例で明らかなごとく、V2O5を添加したち
のは負の温度係数を維持しつつ、密度が向上し製品強度
の改善に効果がある。Table 2 As is clear from these examples, the addition of V2O5 is effective in improving the density and product strength while maintaining a negative temperature coefficient.
本発明の組成について加えておくと、N1フェライトを
選んだのは高周波での電圧拡大率を太きくするに際し、
高電気抵抗とするためである。従って高電気抵抗でかつ
一様な負の温度係数となる元素、例えばCuOを含有さ
せてもよい。さらにCO20は電圧拡大率を一層大きく
するのに効果があるが量が増すに従い、いわゆる第2次
ピークが高温側に大ぎく移動することから、他の成分量
を変えても本発明で規定した0〜80℃の間で一様な負
の温度係数を実現出来ない。Regarding the composition of the present invention, N1 ferrite was chosen because it increases the voltage expansion ratio at high frequencies.
This is to provide high electrical resistance. Therefore, an element having high electrical resistance and a uniform negative temperature coefficient, such as CuO, may be contained. Furthermore, although CO20 is effective in further increasing the voltage magnification ratio, as the amount increases, the so-called secondary peak shifts significantly toward the high temperature side. A uniform negative temperature coefficient cannot be achieved between 0 and 80°C.
B!’20aおよび5iO2fflについては請求の範
囲内で一様な負の温度係数を得られるものである。V
205量に関しては、少ないと密度向上の効果がないの
はもちろんであるが多すぎると異相を生じ易くイTり磁
気特性が劣化する。B! For '20a and 5iO2ffl, uniform negative temperature coefficients can be obtained within the claimed range. V
Regarding the amount of 205, it goes without saying that if it is too small, there will be no effect of improving the density, but if it is too large, different phases are likely to occur and the magnetic properties will deteriorate.
以上の如く本発明の組成物は密度の高い一様な負の温度
係数材を得ることができる。As described above, the composition of the present invention makes it possible to obtain a uniform negative temperature coefficient material with high density.
Claims (1)
(ただし0.8≦X < 1.2.0.01 <V <
0.03 、 1.84242.2でX十V−ト1=
3)で表わされる組成に8!20およびS!02を0.
2≦3 ! 20 a <4wt%、0.2りS i
O2<3wt%、V2O5を上記化学式表示でo、oo
s〜0.04添加し、焼成してなるフェライトで初透磁
率の温度係数が0〜80℃の範囲で一様に負であるこを
特徴とする高周波磁性材料。Chemical formula N i x COy F ez Oa
(However, 0.8≦X<1.2.0.01<V<
0.03, 1.84242.2 x0V-t1=
3) in the composition represented by 8!20 and S! 02 to 0.
2≦3! 20 a <4wt%, 0.2riS i
O2<3wt%, V2O5 in the above chemical formula o, oo
A high-frequency magnetic material, which is made of ferrite obtained by adding 0.04 s to 0.04 and firing, and having a temperature coefficient of initial magnetic permeability that is uniformly negative in the range of 0 to 80°C.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP57233369A JPS59121806A (en) | 1982-12-27 | 1982-12-27 | High-frequency magnetic material |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP57233369A JPS59121806A (en) | 1982-12-27 | 1982-12-27 | High-frequency magnetic material |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS59121806A true JPS59121806A (en) | 1984-07-14 |
Family
ID=16954047
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP57233369A Pending JPS59121806A (en) | 1982-12-27 | 1982-12-27 | High-frequency magnetic material |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS59121806A (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0179466A2 (en) * | 1984-10-24 | 1986-04-30 | Research Development Corporation of Japan | Amorphous ferromagnetic oxides and process for preparing same |
US5346638A (en) * | 1992-09-14 | 1994-09-13 | Murata Manufacturing Co., Inc. | Oxide magnetic material |
EP0891955A1 (en) * | 1997-07-16 | 1999-01-20 | TDK Corporation | Ferrite and inductor |
US6583699B2 (en) | 2000-10-31 | 2003-06-24 | Tdk Corporation | Magnetic material and inductor |
-
1982
- 1982-12-27 JP JP57233369A patent/JPS59121806A/en active Pending
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0179466A2 (en) * | 1984-10-24 | 1986-04-30 | Research Development Corporation of Japan | Amorphous ferromagnetic oxides and process for preparing same |
US5346638A (en) * | 1992-09-14 | 1994-09-13 | Murata Manufacturing Co., Inc. | Oxide magnetic material |
EP0891955A1 (en) * | 1997-07-16 | 1999-01-20 | TDK Corporation | Ferrite and inductor |
US6583699B2 (en) | 2000-10-31 | 2003-06-24 | Tdk Corporation | Magnetic material and inductor |
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