JPS598325Y2 - inductance element - Google Patents
inductance elementInfo
- Publication number
- JPS598325Y2 JPS598325Y2 JP1975053186U JP5318675U JPS598325Y2 JP S598325 Y2 JPS598325 Y2 JP S598325Y2 JP 1975053186 U JP1975053186 U JP 1975053186U JP 5318675 U JP5318675 U JP 5318675U JP S598325 Y2 JPS598325 Y2 JP S598325Y2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- inductance element
- core
- inductance
- current
- 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.)
- Expired
Links
Description
【考案の詳細な説明】
本考案は、磁心に設けた空隙に永久磁石を挿入して磁気
バイアスを与える偏磁形インダクタンス素子に係るもの
である。[Detailed Description of the Invention] The present invention relates to a biased magnetic inductance element that applies a magnetic bias by inserting a permanent magnet into a gap provided in a magnetic core.
チョークコイル等のインダクタンス素子においては、直
流と交流が重畳されるので、直流磁界による磁気飽加を
避けるため、磁心に空隙が設けられていた。In an inductance element such as a choke coil, since direct current and alternating current are superimposed, an air gap has been provided in the magnetic core to avoid magnetic saturation due to the direct current magnetic field.
しかし、磁心に空隙を設けると、インダクタンス値が小
さくなり、これを補なうためには、インダクタンス素子
を大型にしなければならなかった。However, when a gap is provided in the magnetic core, the inductance value decreases, and in order to compensate for this, the inductance element must be made larger.
この欠点を克服するために、軟磁性磁心に永久磁石を挿
入して直流磁界を打消すようにした偏磁形インダクタン
ス素子が考案された。To overcome this drawback, a biased magnetic inductance element was devised in which a permanent magnet is inserted into a soft magnetic core to cancel out the DC magnetic field.
この従来の偏磁形インダクタンス素子の正面断面図及び
側面図を第1図a,l)に示す。A front sectional view and a side view of this conventional biased magnetic inductance element are shown in FIGS. 1a and 1).
磁心は■コア11とEコア12により構威され、Eコア
12の中央脚を両側脚より短くすることにより出来た空
隙部に、磁気バイアスを与える永久磁石13が挿入され
ている。The magnetic core is made up of a core 11 and an E core 12, and a permanent magnet 13 for applying a magnetic bias is inserted into a gap created by making the center leg of the E core 12 shorter than both legs.
永久磁石13の着磁方向は、コイル14に流れる電流が
発生する磁界方向と逆方向である。The direction of magnetization of the permanent magnet 13 is opposite to the direction of the magnetic field generated by the current flowing through the coil 14.
しかし、この従来の偏磁形インダクタンス素子には、チ
ョークコイルを使用した平滑回路内の負荷の短絡又は部
品の故障等により走路電流の数十倍から数百倍の衝撃電
流が流れた場合、永久磁石13に大きな減磁界がかかり
、永久磁石13を減磁してしまうため、インダクタンス
値が小さくなってしまう欠点がある。However, if an impact current of several tens to hundreds of times the running current flows through a smoothing circuit using a choke coil due to a load short circuit or a component failure, this conventional biased magnetic inductance element cannot be used permanently. Since a large demagnetizing field is applied to the magnet 13 and the permanent magnet 13 is demagnetized, there is a drawback that the inductance value becomes small.
本考案は、上記欠点を克服し、インダクタンス値に劣化
の起らないインダクタンス素子を提供することを目的と
するものである。The present invention aims to overcome the above-mentioned drawbacks and provide an inductance element whose inductance value does not deteriorate.
上記目的を達或するために、本考案は、磁心のコイル軸
線方向の中心脚以外の側脚部分に設けた空隙に磁気バイ
アスを与えるための永久磁石を挿入したことを特徴とす
るものである。In order to achieve the above object, the present invention is characterized in that a permanent magnet for applying a magnetic bias is inserted into the air gap provided in the side legs other than the central leg in the coil axis direction of the magnetic core. .
すなわち、本願考案者等は、コイル電流を増大していっ
た場合に磁心が飽和するまでは磁心の各部にほぼ同じ磁
束が流れるが、磁心が飽和すると磁界の増加は主として
コイルの軸線方向の中心脚にのみ生じることに着眼し、
コイル軸線方向の中心脚以外の側脚部分に磁気バイアス
を与える永久磁石を配設して、衝撃電流による減磁界の
影響を制限せしめたものである。In other words, the present inventors have found that when the coil current is increased, almost the same magnetic flux flows through each part of the magnetic core until the magnetic core is saturated, but once the magnetic core is saturated, the increase in magnetic field is mainly caused by Focusing on the fact that it only occurs in the legs,
Permanent magnets that apply magnetic bias are disposed in side leg portions other than the center leg in the axial direction of the coil, thereby limiting the influence of the demagnetizing field caused by the impulse current.
本考案の実施例の正面断面図及び側面図を第2図a,l
)に示す。The front sectional view and side view of the embodiment of the present invention are shown in Figures 2a and l.
).
本考案のインダクタンス素子は、従来の偏磁形インダク
タンス素子とほぼ同じ様に構或されている。The inductance element of the present invention is constructed almost in the same way as a conventional biased magnetic inductance element.
磁心は、■コア11とEコア12から或り、その内部に
コイル14が設けられている。The magnetic core consists of a (1) core 11 and an E core 12, and a coil 14 is provided inside the core.
従来の偏磁形インダクタンス素子と異なる本考案の特徴
は、磁気バイアスを与える永久磁石21.22がEコア
12の両側脚に設けた空隙部に挿入されていることであ
る。A feature of the present invention that differs from conventional biased magnetic inductance elements is that permanent magnets 21 and 22 that provide magnetic bias are inserted into gaps provided on both legs of the E core 12.
いま、この実施例のコイル14に定格電流の数十倍〜数
百倍の衝撃電流が流れた場合1を考えてみる。Now, let us consider a case 1 in which an impact current several tens to hundreds of times the rated current flows through the coil 14 of this embodiment.
衝撃電流により磁心には磁心の飽和磁束密度分の磁界が
発生する。The impact current generates a magnetic field in the magnetic core corresponding to the saturation magnetic flux density of the magnetic core.
軟磁性磁心の場合、小さい電流値で飽和磁束密度分の磁
界が発生するから、当然、コイルに流れる電流による磁
界が発生する。In the case of a soft magnetic core, a magnetic field corresponding to the saturation magnetic flux density is generated with a small current value, so naturally a magnetic field is generated due to the current flowing through the coil.
而してこの実施例に示すような位置に磁気バイアスを与
える永久磁石を設けてあると、衝撃電流が流れても、こ
の永久磁石には、コイルに流れる電流による磁界が加わ
らない。If a permanent magnet that applies a magnetic bias is provided at a position as shown in this embodiment, even if an impact current flows, the magnetic field due to the current flowing through the coil will not be applied to this permanent magnet.
従って永久磁石は減磁されず、インダクタンス値に劣化
が生じない。Therefore, the permanent magnet is not demagnetized and the inductance value does not deteriorate.
尚、永久磁石21.22として、磁心の飽和磁束密度分
の磁界がかかつても減磁しない磁性材料を選択すること
は、勿論必要である。It is of course necessary to select a magnetic material for the permanent magnets 21 and 22 that will not be demagnetized even by a magnetic field equal to the saturation magnetic flux density of the magnetic core.
第3図には、本考案のインダクタンス素子と、従来の偏
磁形インダクタンス素子の直流電流(IDC)に対する
インダクタンスLの変形を示す。FIG. 3 shows the deformation of the inductance L with respect to direct current (IDC) of the inductance element of the present invention and the conventional biased magnetic inductance element.
衝撃電流を流さない場合、従来の偏磁形インダクタンス
素子と本考案のインダクタンス素子は、同様の特性が得
られ、その特性は実線33の様であ.つた。When no impulse current is applied, the conventional biased magnetic inductance element and the inductance element of the present invention have similar characteristics, as shown by the solid line 33. Ivy.
衝撃電流を流した場合、従来の偏磁形インダクタンス素
子は、点線34に示す特性に変化したが、本考案のイン
ダクタンス素子は、衝撃電流を流さない場合の特性を維
持し、インダクタンスの左側移動は生じなかった。When an impact current is applied, the characteristics of the conventional biased magnetic inductance element change to those shown by the dotted line 34, but the inductance element of the present invention maintains the characteristics when no impact current is applied, and the inductance shifts to the left. It did not occur.
以上から明らかなように、本考案によれば、負荷側短絡
又は部品故障等の事故により大きな衝撃電流が流れたと
しても、インダクタンス特性に変化の生じない、信頼性
の高い小型のインダクタンス素子が得られる。As is clear from the above, according to the present invention, a highly reliable small inductance element that does not cause any change in inductance characteristics even if a large shock current flows due to an accident such as a short circuit on the load side or a component failure can be obtained. It will be done.
第1図a,bは各々従来のインダクタンス素子の正面断
面図及び側面図、第2図a,l)は各々本考案の実施例
を示す正面断面図及び側面図、第3図は直流電流に対す
るインダクタンス特性を示す図である。
11 ,12 :磁心、14・・・・・・コイル、13
,21 ,22 :永久磁石。Figures 1a and b are a front sectional view and a side view of a conventional inductance element, Figures 2a and 1) are a front sectional view and a side view of an embodiment of the present invention, respectively, and Figure 3 is a direct current FIG. 3 is a diagram showing inductance characteristics. 11, 12: Magnetic core, 14... Coil, 13
, 21, 22: Permanent magnet.
Claims (1)
設け、該空隙に磁気バイアスを与える永久磁石を挿入し
たことを特徴とするインダクタンス素子。An inductance element characterized in that a gap is provided in a side leg portion of a magnetic core other than the center leg in the coil axis direction, and a permanent magnet is inserted into the gap to apply a magnetic bias.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1975053186U JPS598325Y2 (en) | 1975-04-21 | 1975-04-21 | inductance element |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1975053186U JPS598325Y2 (en) | 1975-04-21 | 1975-04-21 | inductance element |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS51133744U JPS51133744U (en) | 1976-10-28 |
JPS598325Y2 true JPS598325Y2 (en) | 1984-03-15 |
Family
ID=28201470
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP1975053186U Expired JPS598325Y2 (en) | 1975-04-21 | 1975-04-21 | inductance element |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS598325Y2 (en) |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP6265406B2 (en) * | 2013-06-06 | 2018-01-24 | Fdk株式会社 | choke coil |
Family Cites Families (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5041474Y2 (en) * | 1971-10-11 | 1975-11-26 |
-
1975
- 1975-04-21 JP JP1975053186U patent/JPS598325Y2/en not_active Expired
Also Published As
Publication number | Publication date |
---|---|
JPS51133744U (en) | 1976-10-28 |
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