JPS61294805A - External temperature compensation type inductor - Google Patents
External temperature compensation type inductorInfo
- Publication number
- JPS61294805A JPS61294805A JP13588485A JP13588485A JPS61294805A JP S61294805 A JPS61294805 A JP S61294805A JP 13588485 A JP13588485 A JP 13588485A JP 13588485 A JP13588485 A JP 13588485A JP S61294805 A JPS61294805 A JP S61294805A
- Authority
- JP
- Japan
- Prior art keywords
- temperature
- magnetic
- inductance
- curie temperature
- sensitive
- 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
- Coils Or Transformers For Communication (AREA)
Abstract
Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明はコンデンサと組み合わせて共振回路。[Detailed description of the invention] [Industrial application field] The present invention is a resonant circuit in combination with a capacitor.
フィルタ回路、マツチング回路などの電子回路に使用さ
れる温度補償型のインダクタに関する。This invention relates to temperature compensated inductors used in electronic circuits such as filter circuits and matching circuits.
フィルタ回路、マツチング回路1見振回路などに使用さ
れる共振回路の共振周波数f(Hz〕はわせられる。こ
の共振回路の共振周波数fが常に一定で安定するために
は容量CとインダクタンスLが一定でなければならない
。従来から使用されているインダクタは第4図のように
磁性材料よりなる磁気コア2にて閉磁路を形成し。The resonant frequency f (Hz) of a resonant circuit used in filter circuits, matching circuits, etc. is adjusted.In order for the resonant frequency f of this resonant circuit to remain constant and stable, the capacitance C and inductance L must be constant. Conventionally used inductors form a closed magnetic path with a magnetic core 2 made of a magnetic material, as shown in FIG.
その閉磁路中の磁気コア2に巻線4を巻回して形成され
ている。この種のインダクタンスしは磁性材料の形状、
材質、および巻線の巻数Nによって得られ、交流初透磁
率μiacの磁性材料よフなる磁気コアの断面積S、磁
路長tとすればL=μS/1XN2
で表わせる。この式においてインダクタンスLは外気温
度〔℃〕の変化に対しては第5図のように外気温度tの
変化に対して大きくなる傾向にあり、この要因は磁性材
料の透磁率μiacの変化である。すなわち第6図に示
すように外気温度tの変化に対し透磁率μiacの変化
は、温度の上昇に従って増加しキュリー温度に達すると
急激に減小する。従ってインダクタとしての使用温度範
囲はキュリー温度前までであり、インダクタンスしは正
の温度係数を持っている。It is formed by winding a winding 4 around a magnetic core 2 in the closed magnetic path. This kind of inductance is the shape of the magnetic material,
If the cross-sectional area S of a magnetic core made of a magnetic material with an AC initial permeability μiac is determined by the material and the number of turns N of the winding, and the magnetic path length is t, it can be expressed as L=μS/1XN2. In this equation, the inductance L tends to increase as the outside temperature [°C] changes, as shown in Figure 5, and the reason for this is the change in the magnetic permeability μiac of the magnetic material. . That is, as shown in FIG. 6, the change in magnetic permeability μiac with respect to the change in outside temperature t increases as the temperature rises, and sharply decreases when the Curie temperature is reached. Therefore, the temperature range in which it can be used as an inductor is up to the Curie temperature, and the inductance has a positive temperature coefficient.
従来のインダクタは使用される外気温度によってインダ
クタンスLが変化するので外気温度変化の犬なる場所は
共振周波数が不安定で、使用できず、また外気温度変化
の小な場所においては恒温槽内に収納する−ような外気
温度を一定とする手段または、コンデンサCの温度係数
の変化によって補正する手段など精度よく安定に共振周
波数fを保つため電子回路が非常に高価となる欠点があ
った。Conventional inductors have inductance L that changes depending on the outside temperature, so they cannot be used in places where the outside temperature changes because the resonance frequency is unstable, and they cannot be used in places where the outside temperature changes little. In order to maintain the resonant frequency f accurately and stably, such as means for keeping the outside air temperature constant, or means for correcting it by changing the temperature coefficient of the capacitor C, the electronic circuitry is extremely expensive.
本発明は従来のかかる欠点を除き、高いキュリー温度の
磁性材よりなる磁気コア2の一部に低キユリ一温度の異
なる複数種の感温磁性体を挿入して閉磁路全形成し、こ
の磁気コア2に巻線4を巻回し外気温度tの変化に対し
て安定なインダクタンスLの値を有する外気温度補償型
のインダクタである。The present invention eliminates such drawbacks of the conventional technology and forms a closed magnetic path by inserting a plurality of types of temperature-sensitive magnetic materials with different low Curie temperatures into a part of the magnetic core 2 made of a magnetic material with a high Curie temperature. This is an outside temperature compensated inductor in which a winding 4 is wound around a core 2 and the inductance L value is stable against changes in outside temperature t.
複数種のキュリー温度の低い感温磁性体は外気温度上が
上昇する毎にキュリー温度と透磁率を変化の大なる向き
に移動変化させ、インダクタンスLの値の変化を小さく
する。A plurality of types of temperature-sensitive magnetic materials having a low Curie temperature move and change the Curie temperature and magnetic permeability in the direction of a larger change each time the outside air temperature rises, thereby reducing a change in the value of the inductance L.
本発明の実施例は第1図に示すように中央の脚部1を他
の脚部2の長さより短いE型磁気コア2を突き合わせ、
中央脚部1間に空隙部3を設ける。この空隙部3内に2
種以上の異なるキュリー温度を有する感温磁性体よりな
る磁気コアを挿入し閉磁路とし、この中央脚部1に巻線
4を巻回し外気温度補償型のインダクタが形成される。In the embodiment of the present invention, as shown in FIG. 1, a central leg 1 is butted against an E-shaped magnetic core 2 whose length is shorter than the other legs 2.
A gap 3 is provided between the central legs 1. 2 in this cavity 3
A magnetic core made of temperature-sensitive magnetic materials having different Curie temperatures or more is inserted to form a closed magnetic circuit, and a winding 4 is wound around the central leg 1 to form an outside temperature compensated inductor.
このインダクタの空隙部3に挿入される感温磁性体はキ
ュリー温度がそれぞれ異り、その動作は第2図の外気温
度tと透磁率μiacとの関係を示す曲線のように、ま
ず低温より外気温度が上昇して曲線aの温度範囲にある
感温磁性体がキュリー温度に達すると急激に透磁率μi
acが減少する。しかし曲線すの温度範囲に達し同様の
現象を生ずるので磁気コア2と組み合わせてもインダク
タンスLの値は感温磁性体のキュIJ 一温度において
のみ減少し、この感温磁性体のキュリー温度以上におい
て減少した値はつぎの感温磁性体に移行し変化の少ない
透磁率μiacが得られる。また第6図に示すように本
発明のインダクタにおける外気温度tの変化とインダク
タンスLの値の変化を示す。図に示すように曲線メは従
来のインダクタにおけるように正の温度す
係数をもつ。また曲線ノは本発明による一20〜50℃
の感温磁性体を使用し1曲線Cは一20〜+80℃の感
温磁性体を使用したインダクタンスの値で負の温度係数
を持ちその変化は従来のものに比べて少ない。The temperature-sensitive magnetic bodies inserted into the air gap 3 of this inductor have different Curie temperatures, and their operation is as shown in the curve showing the relationship between the outside temperature t and the magnetic permeability μiac in Figure 2. When the temperature rises and the temperature-sensitive magnetic material in the temperature range of curve a reaches the Curie temperature, the magnetic permeability μi suddenly decreases.
ac decreases. However, since the temperature range of the curve is reached and a similar phenomenon occurs, even when combined with magnetic core 2, the value of inductance L decreases only at one temperature of the temperature-sensitive magnetic material's Curie temperature, and above the Curie temperature of this temperature-sensitive magnetic material. The decreased value is transferred to the next temperature-sensitive magnetic material, and a magnetic permeability μiac with little change is obtained. Further, as shown in FIG. 6, changes in the outside temperature t and changes in the value of the inductance L in the inductor of the present invention are shown. As shown in the figure, the curve has a positive temperature coefficient as in conventional inductors. In addition, the curve is -20 to 50℃ according to the present invention.
1 curve C is an inductance value using a temperature-sensitive magnetic material of -20 to +80°C, which has a negative temperature coefficient, and its change is smaller than that of the conventional one.
以上に述べたように本発明によれば、温度係数は負であ
り外気温度tの変化に対してインダクタンスLの値の変
化の小さいインダクタが得られ、外気温度tに対して安
定した共振周波数を持つ共振回路、フィルタ回路などの
電子回路が形成される。As described above, according to the present invention, an inductor with a negative temperature coefficient and a small change in the value of inductance L with respect to changes in outside temperature t can be obtained, and a stable resonant frequency with respect to outside temperature t can be obtained. Electronic circuits such as resonant circuits and filter circuits are formed.
第1図は本発明のインダクタの実施例の縦断正面図、第
2図は本発明による外気温度と各種の温度範囲の感温磁
性体の透磁率の変化を示す曲線図、第3図は本発明によ
るインダクタと従来のインダクタのインダクタンス値と
外気温度との関係を示す曲線図、第4図は従来のインダ
クタの縦断面図(a)と外観斜視図(b)、第5図は従
来のインダクタのインダクタンス値と外気温度との関係
を示す曲線図、第6図は感温磁性体の透磁率と外気温度
との関係を示す曲線図である。
なお
2:磁気コア、3:空隙部、4:巻線。
第1図
第2図
(a)(1))
4 第4図FIG. 1 is a longitudinal sectional front view of an embodiment of the inductor of the present invention, FIG. 2 is a curve diagram showing changes in magnetic permeability of the temperature-sensitive magnetic material in various temperature ranges and outside air temperature according to the present invention, and FIG. 3 is a diagram of the present invention. A curve diagram showing the relationship between the inductance value and outside temperature of the inductor according to the invention and the conventional inductor, FIG. 4 is a vertical cross-sectional view (a) and an external perspective view (b) of the conventional inductor, and FIG. 5 is the conventional inductor. FIG. 6 is a curve diagram showing the relationship between the inductance value and the outside temperature. FIG. 6 is a curve diagram showing the relationship between the magnetic permeability of the temperature-sensitive magnetic material and the outside temperature. Note that 2: magnetic core, 3: gap, 4: winding. Figure 1 Figure 2 (a) (1)) 4 Figure 4
Claims (1)
閉磁路の一部に低キュリー温度の異なる複数種の感温磁
性体を挿入し前記磁気コアに巻線したことを特徴とする
外気温度補償型のインダクタ。1. Outdoor temperature compensation characterized in that a plurality of types of temperature-sensitive magnetic materials having different low Curie temperatures are inserted into a part of the closed magnetic circuit of a magnetic core made of a magnetic material having a high Curie temperature and wound around the magnetic core. type inductor.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP13588485A JPS61294805A (en) | 1985-06-24 | 1985-06-24 | External temperature compensation type inductor |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP13588485A JPS61294805A (en) | 1985-06-24 | 1985-06-24 | External temperature compensation type inductor |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS61294805A true JPS61294805A (en) | 1986-12-25 |
Family
ID=15162034
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP13588485A Pending JPS61294805A (en) | 1985-06-24 | 1985-06-24 | External temperature compensation type inductor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61294805A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN103208352A (en) * | 2013-03-15 | 2013-07-17 | 沈阳工业大学 | Novel power transformer with direct current magnetic bias suppression function on basis of magnetic temperature compensation |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS49129U (en) * | 1972-04-08 | 1974-01-05 |
-
1985
- 1985-06-24 JP JP13588485A patent/JPS61294805A/en active Pending
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS49129U (en) * | 1972-04-08 | 1974-01-05 |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN103208352A (en) * | 2013-03-15 | 2013-07-17 | 沈阳工业大学 | Novel power transformer with direct current magnetic bias suppression function on basis of magnetic temperature compensation |
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