JPS5922306A - Magnetic core for discharge lamp stabilizer - Google Patents
Magnetic core for discharge lamp stabilizerInfo
- Publication number
- JPS5922306A JPS5922306A JP57132783A JP13278382A JPS5922306A JP S5922306 A JPS5922306 A JP S5922306A JP 57132783 A JP57132783 A JP 57132783A JP 13278382 A JP13278382 A JP 13278382A JP S5922306 A JPS5922306 A JP S5922306A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic core
- mold
- pressing
- discharge lamp
- angle
- 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
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F27/00—Details of transformers or inductances, in general
- H01F27/24—Magnetic cores
- H01F27/255—Magnetic cores made from particles
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Powder Metallurgy (AREA)
Abstract
Description
【発明の詳細な説明】
従来の放電灯安定器用磁気コアは、ケイ素鋼板をプレス
により打ち抜き後、積層して磁気コアと成しているため
に、形状的に制約を受け、角形状、角型ボビン等の制約
を脱し得ない欠点があった。本発明は上記欠点を解決す
るもので、関してなされたものである。[Detailed Description of the Invention] Conventional magnetic cores for discharge lamp ballasts are formed by punching silicon steel plates with a press and then laminating them to form the magnetic core. Therefore, there are restrictions on the shape, such as rectangular or rectangular shapes. There was a drawback that it was impossible to escape from the restrictions of the bobbin, etc. The present invention has been made to solve the above-mentioned drawbacks.
以後、図をもとにして説明すると、図1で例示するよう
に、プレス方向(抜き方向)に対して、側面部が平行で
ある場合、当該磁気コアが金型に密着し、抜き取るのが
非常に困難であり、又第一回目のプレス後、当該磁気コ
アを金型よら膨張するので、サイジング(再圧縮)する
B寺に、第一回目と同じ金型が使用できないため、別に
サイジング用の金型が心安であった。本発明は例えば図
2のような形状にすると、プレス方向(抜き方向)に対
して側面部に、鉛直線に対するチー・ぐ−の角度を、1
°以下にすると抜き取り易くするのに効果がなく、又2
0°以上にすると安定器に組立だ時、強度的に弱くなる
ので、ノ0レス方向(抜き方向)に対して側面部に、鉛
直線にえすして、1°〜2000角度のチー斗−を設け
、その為に、第一回目のフ0レス時の抜き取りが容易に
なり、金型に当該磁気コアが密着して離れなくなったり
することがなくなる。又第一回目のプレス後、当該磁気
コアを抜き敗った時、わずかに膨張しても、第一回目の
フ0レスに使用した同じ金型を使って、サイジング(再
圧縮)が可能である。ここで、磁気コアの性能を左右す
るものの一つに透磁率があり、透磁率が上昇すると磁気
コアの性能がよく、なる。磁気コアの密度が十列すると
、それにともなって透磁率も一上列するので、サイジン
グ(再圧縮)により、当該磁気コアの性能が向上するも
のである。Hereinafter, an explanation will be given based on the drawings. As illustrated in Fig. 1, when the side surface is parallel to the pressing direction (extraction direction), the magnetic core is in close contact with the mold and it is difficult to extract it. It is very difficult to press, and since the magnetic core expands from the mold after the first pressing, the same mold as the first time cannot be used for sizing (recompression), so a separate sizing mold is used. The mold was safe. In the present invention, for example, when the shape is as shown in FIG.
If it is less than °, it will not be effective in making it easier to remove, and
If the angle is more than 0°, the strength will be weakened when assembled into the ballast, so insert a chi-toe at an angle of 1° to 2000 on the side part in the vertical line with respect to the direction of removal (extraction direction). This makes it easier to remove the magnetic core during the first freeing process, and prevents the magnetic core from coming into close contact with the mold and becoming unable to separate from it. In addition, even if the magnetic core expands slightly after the first pressing, it can be sized (recompressed) using the same mold used for the first pressing. be. Here, one of the factors that influences the performance of the magnetic core is magnetic permeability, and as the magnetic permeability increases, the performance of the magnetic core improves. When the density of the magnetic core increases to 10, the permeability also increases, so sizing (recompression) improves the performance of the magnetic core.
次に、図Iに例示するように、磁気コア基底部内面中央
に窪みのないものと、同じ材料で、同じ粉末冶金法で、
同じ条件で直方体状のものを製作L、それを削り出して
作った同型の磁気コアとを比較すると、金型で図1に示
すように作った磁気コアの方が性能が低下した。Next, as illustrated in Figure I, a magnetic core without a depression at the center of the inner surface of the base is made of the same material and by the same powder metallurgy method.
A rectangular parallelepiped-shaped core L was manufactured under the same conditions, and when compared with a magnetic core of the same type made by cutting it, the performance of the magnetic core made using a mold as shown in FIG. 1 was lower.
とれは、中央脚部1と両端脚部2との間の密度に不均一
が生じ、そのために透磁率が部分によって異なるためで
ある。又この密度の不均一のために脚部に亀裂が生じる
。しかるに、図2に例示するように、コア基底内面中央
に窪み4を設けると、中央脚部1の密度が上昇し、両端
脚部2と中央脚部1の密度が均一化し、当該磁気コアの
密度が全体として上昇し、従って透磁率が上昇して、磁
気コアとしての性能が格段と向上した。又密度が均一化
することによって金型より抜き取った直後に発生する脚
部の亀裂がなくなる。又図5の磁気コアの内側の点線で
示すように、磁束は角張って流れるものではなく6、コ
アの各角部分は円弧を描いて流れるものであって7、図
2に例示するように、基底部内面中央に窪み4を設けて
も、磁気コアとしての性能は殆んど変化せず、窪みの分
だけ材料の削減になり、軽量化及びコストダウンにつな
がるものである。さらに、安定器として組立てる際に、
ベースやカバーで被う時の中心の位置決めにもなる。This is because the density between the central leg portion 1 and both end leg portions 2 is non-uniform, and as a result, the magnetic permeability differs depending on the portion. This non-uniform density also causes cracks in the legs. However, as illustrated in FIG. 2, when a depression 4 is provided at the center of the inner surface of the base of the core, the density of the center leg 1 increases, the density of both end legs 2 and the center leg 1 becomes uniform, and the density of the magnetic core increases. The overall density has increased, and therefore the magnetic permeability has increased, and the performance as a magnetic core has been significantly improved. Also, by making the density uniform, cracks in the legs that occur immediately after being removed from the mold are eliminated. Also, as shown by the dotted line inside the magnetic core in FIG. 5, the magnetic flux does not flow in an angular manner6, but flows in an arc at each corner of the core7, as illustrated in FIG. Even if the recess 4 is provided at the center of the inner surface of the base, the performance as a magnetic core hardly changes, and the amount of material is reduced by the amount of the recess, leading to weight reduction and cost reduction. Furthermore, when assembled as a stabilizer,
It can also be used to determine the center position when covering with a base or cover.
次に、先に述べたように、磁束はコアの各角部分で円弧
を描いて流れるため7、各角部分及び各稜線部を削り取
っても磁気的にあ1り影響を与えない。従って各角部分
の全部或いは一部に、又各稜線部の全部或いは一部にR
をつけることによって、材料を削減し、しかも安定器の
組立ての際或いは、照明器具の組立時に発生する衝撃に
おいて安定器が破損しないものである。Next, as described above, since the magnetic flux flows in an arc at each corner of the core 7, even if each corner and each ridgeline are removed, there will be no magnetic effect. Therefore, all or part of each corner part and all or part of each ridgeline part are rounded.
By attaching the ballast, the amount of material can be reduced, and the ballast will not be damaged by shocks that occur when assembling the ballast or when assembling the lighting equipment.
このように本発明は、粉末冶金法による放電灯安定器用
磁気コアにおいて、磁気的に好結果をもたらすことはむ
ろんのこと、材料の削減を行ない、従って安定器の軽量
化に役立ち、近年ともすると照明器具が大型化する上に
、少しでも器具を小型軽量化でき、安価に照明器具を提
供できるなどの多くの特徴を有するものである。As described above, the present invention not only brings about good magnetic results in a magnetic core for a discharge lamp ballast using a powder metallurgy method, but also reduces the amount of material used, and therefore helps to reduce the weight of the ballast, which has become popular in recent years. In addition to increasing the size of lighting equipment, it has many features such as being able to reduce the size and weight of the equipment even a little, and providing lighting equipment at low cost.
図面は本発明放電灯用安定器の磁気コアの一実施例を示
すものであって、図1、図2は磁気コアの断面図、図3
、図4は同斜視図、図5は同模式図。
1・・・・中央脚部 2・・・・両端脚部3・・
・・基底中央部 4・・・・基底内面中央の窪み5
・・・・稜線部
特許出願人 黒井興産株式会社The drawings show an embodiment of the magnetic core of the ballast for a discharge lamp according to the present invention, and FIGS. 1 and 2 are cross-sectional views of the magnetic core, and FIG. 3 is a cross-sectional view of the magnetic core.
, FIG. 4 is a perspective view of the same, and FIG. 5 is a schematic diagram of the same. 1...Central leg 2...Both end legs 3...
・Basal central part 4 ・・Concavity 5 in the center of the basal inner surface
...Ridge patent applicant Kuroi Kosan Co., Ltd.
Claims (3)
おいて、粉末冶金法で、粉末を圧縮成型する過程で、プ
レス方向(抜き方向)に対して側面部に、鉛直線に対し
て1°〜20°の角度のチー・ぐ−を設けることを特徴
とする放電灯用安定器の磁気コア。(1) In a magnetic core for a discharge lamp ballast made by powder metallurgy, in the process of compression molding powder by powder metallurgy, the side part with respect to the pressing direction (pull direction) is 1° to 20° with respect to the vertical line. A magnetic core for a ballast for a discharge lamp, characterized in that it is provided with a tip at an angle of .
て、当該磁気コアの基底部内面中央に、舒みを設けた特
許請求の範囲第一項記載の放電灯用安定器の磁気コア。(2) A magnetic core for a ballast for a discharge lamp according to claim 1, wherein the magnetic core for a ballast for a discharge lamp is made by a powder metallurgy method, and a stub is provided at the center of the inner surface of the base of the magnetic core.
て、当該磁気コアの各角部の全て及びその一部にRをつ
け、又当該磁気コアの各稜線部の全て、或いはその一部
を曲面とした特許請求の範囲第一項記載の放電灯用安定
器の磁気コア。(3) In a magnetic core for a discharge lamp ballast made by powder metallurgy, all or part of each corner of the magnetic core is rounded, and all or part of each ridgeline of the magnetic core is curved. A magnetic core of a ballast for a discharge lamp according to claim 1.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP57132783A JPS5922306A (en) | 1982-07-28 | 1982-07-28 | Magnetic core for discharge lamp stabilizer |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP57132783A JPS5922306A (en) | 1982-07-28 | 1982-07-28 | Magnetic core for discharge lamp stabilizer |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS5922306A true JPS5922306A (en) | 1984-02-04 |
JPH0522370B2 JPH0522370B2 (en) | 1993-03-29 |
Family
ID=15089435
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP57132783A Granted JPS5922306A (en) | 1982-07-28 | 1982-07-28 | Magnetic core for discharge lamp stabilizer |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5922306A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2008085163A (en) * | 2006-09-28 | 2008-04-10 | Hitachi Metals Ltd | Ferrite core |
JP2012248899A (en) * | 2011-03-30 | 2012-12-13 | Sumitomo Electric Ind Ltd | Outer core manufacturing method, outer core, and reactor |
CN102930959A (en) * | 2011-08-08 | 2013-02-13 | 株式会社神户制钢所 | A press powder magnetic core component used for a winding component, producing method, press powder magnetic core used for a winding component, and a winding component |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5318066A (en) * | 1976-08-03 | 1978-02-18 | Meidensha Electric Mfg Co Ltd | Method for molding pulverulent body |
JPS5429448U (en) * | 1977-07-31 | 1979-02-26 |
-
1982
- 1982-07-28 JP JP57132783A patent/JPS5922306A/en active Granted
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5318066A (en) * | 1976-08-03 | 1978-02-18 | Meidensha Electric Mfg Co Ltd | Method for molding pulverulent body |
JPS5429448U (en) * | 1977-07-31 | 1979-02-26 |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2008085163A (en) * | 2006-09-28 | 2008-04-10 | Hitachi Metals Ltd | Ferrite core |
JP2012248899A (en) * | 2011-03-30 | 2012-12-13 | Sumitomo Electric Ind Ltd | Outer core manufacturing method, outer core, and reactor |
CN102930959A (en) * | 2011-08-08 | 2013-02-13 | 株式会社神户制钢所 | A press powder magnetic core component used for a winding component, producing method, press powder magnetic core used for a winding component, and a winding component |
Also Published As
Publication number | Publication date |
---|---|
JPH0522370B2 (en) | 1993-03-29 |
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