JPS6311822Y2 - - Google Patents

Info

Publication number
JPS6311822Y2
JPS6311822Y2 JP151279U JP151279U JPS6311822Y2 JP S6311822 Y2 JPS6311822 Y2 JP S6311822Y2 JP 151279 U JP151279 U JP 151279U JP 151279 U JP151279 U JP 151279U JP S6311822 Y2 JPS6311822 Y2 JP S6311822Y2
Authority
JP
Japan
Prior art keywords
yoke
magnet
magnetic
magnetic circuit
height
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
Application number
JP151279U
Other languages
Japanese (ja)
Other versions
JPS55102289U (en
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed filed Critical
Priority to JP151279U priority Critical patent/JPS6311822Y2/ja
Priority to US06/096,399 priority patent/US4412104A/en
Publication of JPS55102289U publication Critical patent/JPS55102289U/ja
Application granted granted Critical
Publication of JPS6311822Y2 publication Critical patent/JPS6311822Y2/ja
Expired legal-status Critical Current

Links

Landscapes

  • Audible-Bandwidth Dynamoelectric Transducers Other Than Pickups (AREA)

Description

【考案の詳細な説明】 本考案は角型ヨークを用いる内磁型スピーカ用
磁気回路に関する。
[Detailed Description of the Invention] The present invention relates to a magnetic circuit for an internal magnetic type speaker using a rectangular yoke.

従来内磁型スピーカ用磁気回路のマグネツトと
してアルニコ磁石が用いられて来ているが、従来
のアルニコ磁石を用いた最適磁気回路に実願48−
65430があるが、アルニコ磁石の主成分であるCo
が最近入手難であることからフエライト磁石へ応
用がなされている。しかしアルニコ磁石とフエラ
イト磁石の磁気特性の差異により同等の特性を求
めるならばアルニコ磁石よりフエライト磁石の方
が大きくならざるを得ず、しかもヨークまでも大
きくする必要が生じるなどの問題点があつた。
Conventionally, alnico magnets have been used as magnets in magnetic circuits for internal magnet type speakers, but it has been proposed to develop an optimal magnetic circuit using conventional alnico magnets.
65430, but Co is the main component of alnico magnets.
Since it is difficult to obtain ferrite magnets recently, it has been applied to ferrite magnets. However, due to the difference in magnetic properties between alnico magnets and ferrite magnets, if the same characteristics were to be obtained, ferrite magnets had to be larger than alnico magnets, and even the yoke had to be larger. .

本考案は上記の問題点を解決すると同時に、内
磁型スピーカ用磁気回路の磁石にフエライト磁石
を用いた場合の磁気回路の最適形状を決めた磁気
回路を提供するものである。
The present invention solves the above-mentioned problems and at the same time provides a magnetic circuit in which the optimum shape of the magnetic circuit is determined when a ferrite magnet is used as the magnet of the magnetic circuit for an internal magnetic type speaker.

本考案の実施例を図面により説明すると、第1
図aは、本考案の内磁型スピーカ用磁気回路の上
面図、bはaの縦断面図で、1は一方向両端部が
開放のヨークで上部に貫通孔2が設けられており
3はヨーク1の内周底面に取付られた角柱状のフ
エライト磁石、4は同磁石上に取付られた円錐状
または角錐状のセンターポールである。なおセン
ターポール4とヨーク孔2との空隙に上下移動可
能に支持されるボイスコイル(図示せず)がある
ことは言うまでもない。第1図ではtyはヨークの
厚さ、hyおよびhmはそれぞれヨークの高さおよ
びフエライト磁石の高さ、wyおよびw□mはそれ
ぞれヨークの幅およびフエライト磁石の寸法を示
す。フエライト磁石における透磁率は1.05〜1.10
程度であるため、磁石からヨークへの磁束の内部
漏洩がアルニコ磁石より小さく、内部漏洩の主体
はセンターポールからヨークへの段階で問題とな
るもので、フエライト磁石はアルニコの約1/2程
度の残留磁束密度(Bg)しかない。このため所
定のBgを得るにはマグネツトの断面積を大きく
しなければならない。以上のことによりヨーク内
積一杯のマグネツト断面積を有するマグネツトを
使用する必要がある。
The first embodiment of the present invention will be explained with reference to the drawings.
Figure a is a top view of the magnetic circuit for an internal magnet type speaker according to the present invention, and figure b is a longitudinal cross-sectional view of figure a, in which 1 is a yoke with both ends open in one direction, and a through hole 2 is provided in the upper part. A prismatic ferrite magnet is attached to the inner bottom surface of the yoke 1, and 4 is a conical or pyramidal center pole attached to the magnet. It goes without saying that there is a voice coil (not shown) supported in the gap between the center pole 4 and the yoke hole 2 so as to be movable up and down. In FIG. 1, ty is the thickness of the yoke, hy and hm are the height of the yoke and the height of the ferrite magnet, respectively, and wy and w m are the width of the yoke and the dimensions of the ferrite magnet, respectively. Magnetic permeability in ferrite magnets is 1.05-1.10
Therefore, the internal leakage of magnetic flux from the magnet to the yoke is smaller than that of alnico magnets, and the main problem of internal leakage is from the center pole to the yoke. There is only residual magnetic flux density (Bg). Therefore, in order to obtain a predetermined Bg, the cross-sectional area of the magnet must be increased. Due to the above, it is necessary to use a magnet having a cross-sectional area that is equal to the inner volume of the yoke.

これ等から構成する磁気回路を使用して重要と
なるマグネツト高さhmヨーク高さhyの比率を検
討した結果を第2図に示す。この時の設定条件と
しては、角型ヨークにてty=4(単位m/m)、
wy48,w□m□35、φp,φ14、tg=0.75でありこ
れらを比率を変化させて行くと、第2図に示す如
く、hy/hmが2.4〜2.6の時のBgが最大値を有す
ることが判明した。以上の結果からヨーク高さに
対するマグネツト高さ2.4〜2.6の間を使用すれば
残溜磁束密度が最高特性で利用出来るものであ
る。
FIG. 2 shows the results of examining the important ratio of magnet height hm to yoke height hy using a magnetic circuit constructed from these components. The setting conditions at this time are ty = 4 (unit: m/m) for a square yoke.
wy48, w□m□35, φp, φ14, tg=0.75, and by changing the ratio of these, Bg has the maximum value when hy/hm is 2.4 to 2.6, as shown in Figure 2. It has been found. From the above results, if the magnet height relative to the yoke height is between 2.4 and 2.6, the residual magnetic flux density can be utilized with the best characteristics.

上記実施例から明らかなように、角型のフエラ
イト磁石を用いることにより従来使用の角型ヨー
クを変更することもなくそのまゝ使用することが
出来、しかも磁気漏洩が大巾に低減出来るもので
ある。また空隙磁束密度も従来そ同等の特性を得
ることが出来る等、その工業的効果は大なるもの
である。
As is clear from the above examples, by using a square ferrite magnet, the conventional square yoke can be used as is without any modification, and magnetic leakage can be greatly reduced. be. In addition, the air gap magnetic flux density can be obtained with characteristics equivalent to those of the conventional method, and its industrial effects are great.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図aは、本考案の内磁型スピーカ用磁気回
路の上面図、bはaの縦断面図、第2図は空隙磁
束密度の説明図である。
FIG. 1a is a top view of the magnetic circuit for an internal magnet type speaker of the present invention, b is a longitudinal sectional view of a, and FIG. 2 is an explanatory diagram of the air gap magnetic flux density.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 高さ及び寸法幅を有する一方向両端部が開放の
角型ヨークに上部へ貫通孔を有し該ヨークの内周
底面に内容量が最大の永久磁石を取付けた内磁型
スピーカ用磁気回路において、前記ヨーク高さ
hyと永久磁石hmとの比を2.4〜2.6<hy/hm<と
し、該永久磁石に角柱状フエライト磁石を用いた
ことを特徴とする内磁型スピーカ用磁気回路。
In a magnetic circuit for an internally magnetic speaker, which has a square yoke with a height and width and is open at both ends in one direction, has a through hole at the top, and a permanent magnet with the largest internal capacity is attached to the bottom of the inner periphery of the yoke. , the yoke height
1. A magnetic circuit for an internal magnetic speaker, characterized in that the ratio of hy to a permanent magnet hm is 2.4 to 2.6<hy/hm<, and a prismatic ferrite magnet is used as the permanent magnet.
JP151279U 1978-11-24 1979-01-10 Expired JPS6311822Y2 (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP151279U JPS6311822Y2 (en) 1979-01-10 1979-01-10
US06/096,399 US4412104A (en) 1978-11-24 1979-11-21 Rectangular magnetic circuit for speaker

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP151279U JPS6311822Y2 (en) 1979-01-10 1979-01-10

Publications (2)

Publication Number Publication Date
JPS55102289U JPS55102289U (en) 1980-07-16
JPS6311822Y2 true JPS6311822Y2 (en) 1988-04-06

Family

ID=28803729

Family Applications (1)

Application Number Title Priority Date Filing Date
JP151279U Expired JPS6311822Y2 (en) 1978-11-24 1979-01-10

Country Status (1)

Country Link
JP (1) JPS6311822Y2 (en)

Also Published As

Publication number Publication date
JPS55102289U (en) 1980-07-16

Similar Documents

Publication Publication Date Title
JPS6311822Y2 (en)
US3971054A (en) Method and apparatus for magnetizing permanent magnet in magnetic structure
JPH0534797U (en) Magnetic circuit for speaker
JP2567822Y2 (en) Magnetic circuit for speaker
JPS635348Y2 (en)
JPS5931110Y2 (en) electrodynamic speaker
JPS5838713Y2 (en) Magnetic circuit structure of permanent magnet for speaker
JP3207697B2 (en) Repulsion magnetic circuit of speaker
JPS635347Y2 (en)
JPS581036Y2 (en) Speaker magnetic circuit
JPS5880999A (en) Loud speaker
JPS6022712Y2 (en) Speaker magnetic circuit
JPH0570097U (en) Inner magnet type magnetic circuit
JPH062895U (en) Magnetic circuit for speaker
JPS5815969U (en) Objective lens for electron beam equipment
JPH0412795U (en)
JPS593699U (en) electromagnetic speaker
JPS5876294U (en) Low leakage magnetic flux speaker
JPS60150893U (en) Magnetic circuit for speakers
JPH048598U (en)
JPH0417678U (en)
JPH0257322B2 (en)
JPH059099U (en) Dynamic type acoustic parts
JPS5925565A (en) Moving coil type drive device
JPH0613295U (en) Oval speaker