JPH0422637Y2 - - Google Patents
Info
- Publication number
- JPH0422637Y2 JPH0422637Y2 JP1982038236U JP3823682U JPH0422637Y2 JP H0422637 Y2 JPH0422637 Y2 JP H0422637Y2 JP 1982038236 U JP1982038236 U JP 1982038236U JP 3823682 U JP3823682 U JP 3823682U JP H0422637 Y2 JPH0422637 Y2 JP H0422637Y2
- Authority
- JP
- Japan
- Prior art keywords
- magnet
- plate
- magnetic
- speaker
- magnetic circuit
- 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
- 230000005415 magnetization Effects 0.000 claims description 7
- 230000004907 flux Effects 0.000 description 18
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 6
- 229910000828 alnico Inorganic materials 0.000 description 3
- 230000005520 electrodynamics Effects 0.000 description 3
- 229910052742 iron Inorganic materials 0.000 description 3
- 230000007423 decrease Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 239000012141 concentrate Substances 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
Landscapes
- Audible-Bandwidth Dynamoelectric Transducers Other Than Pickups (AREA)
Description
【考案の詳細な説明】
本考案は音響機器に使用する動電型スピーカの
磁気回路に関し、特に寸法の制約があつても十分
なギヤツプ内磁束密度が得られる様にし良好なス
ピーカ駆動なし得る様にしたものである。[Detailed description of the invention] The present invention relates to a magnetic circuit for an electrodynamic speaker used in audio equipment, and is designed to obtain a sufficient magnetic flux density in the gap and achieve good speaker drive even when there are dimensional restrictions. This is what I did.
従来、所謂内磁型磁気回路を有するスピーカ1
として例えば第1図に示す如きものがあつた。こ
の第1図において、2は純鉄製のヨークを示し、
このヨーク2内にはマグネツト3が設けられてい
る。このマグネツト3はアルニコ製の円柱形状の
ものでマグネツト3の軸線方向に着磁されてお
り、S極側の端部の円形平面3a全面がヨーク2
の底部内面2aに互いに中心軸に合わせて当接さ
れて固着されている。マグネツト3のN極側の端
部の円形平面に、底面4aの直径をヨーク2の開
口部の径の長さから磁気ギヤツプ5の幅として必
要な分を差し引いた長さとし厚さをヨーク2の肉
厚と同一の厚さとした円板状のトツププレート4
が設けられている。之等マグネツト3、ヨーク
2、磁気ギヤツプ5、トツププレート4により磁
気回路が構成され、磁気ギヤツプ5内のボイスコ
イル6に流れる電流に応じて振動板7がマグネツ
ト3の着磁方向と同一方向に前後に振動して音声
を得る如くなされている。かかる内磁型磁気回路
を有するスピーカ1にあつて磁気ギヤツプ5内の
磁束密度を高くしようとするとマグネツト3の径
を大きくし大型化しなければならない。この大型
化の際、磁束を集中させるためにセンターポール
10を導入する必要が生じるが、かかるセンター
ポール10に係わる磁束の漏れにより磁束利用率
が減少してしまうため、この磁束の漏れを補う意
味で更にマグネツト3を大きめにする必要があつ
た。従つて、磁気ギヤツプ5内を高磁束密度にし
ようとすればスピーカの磁気回路の幅方向及び奥
行方向についての大型化が必要であり、かかる磁
気回路について幅あるいは奥行に寸法上の制約が
ある場合には所望の十分な磁気ギヤツプ5内の磁
束密度を得ようとしても不可能となつてしまう場
合も生ずるという構造に係わる欠点があつた。ま
た、高価なアルニコをマグネツト3の材料として
いるので大型化したスピーカが大変高価になつて
しまうという欠点もあつた。 Conventionally, a speaker 1 having a so-called internal magnetic type magnetic circuit
For example, there was something like the one shown in Figure 1. In this Fig. 1, 2 indicates a yoke made of pure iron,
A magnet 3 is provided within the yoke 2. This magnet 3 is made of alnico and has a cylindrical shape, and is magnetized in the axial direction of the magnet 3, and the entire circular plane 3a at the end on the S pole side is connected to the yoke 2.
They are abutted and fixed to the bottom inner surface 2a of the base 2a, aligned with each other along their central axes. On the circular plane of the N-pole side end of the magnet 3, set the diameter of the bottom surface 4a to the length of the opening of the yoke 2 minus the width required for the magnetic gap 5, and set the thickness of the yoke 2. Disc-shaped top plate 4 with the same thickness as the wall thickness
is provided. A magnetic circuit is constituted by the magnet 3, yoke 2, magnetic gap 5, and top plate 4, and the diaphragm 7 moves in the same direction as the magnetization direction of the magnet 3 according to the current flowing through the voice coil 6 in the magnetic gap 5. It vibrates back and forth to produce sound. In order to increase the magnetic flux density within the magnetic gap 5 in the speaker 1 having such an internal magnet type magnetic circuit, the diameter of the magnet 3 must be increased to increase its size. When increasing the size, it becomes necessary to introduce a center pole 10 in order to concentrate the magnetic flux, but since the magnetic flux utilization rate decreases due to the leakage of magnetic flux related to the center pole 10, it is necessary to compensate for this leakage of magnetic flux. So it was necessary to make the magnet 3 larger. Therefore, in order to achieve a high magnetic flux density inside the magnetic gap 5, it is necessary to increase the size of the speaker's magnetic circuit in the width and depth directions, and if there are dimensional restrictions on the width or depth of such a magnetic circuit. The structure had a drawback in that it was sometimes impossible to obtain a desired and sufficient magnetic flux density within the magnetic gap 5. Furthermore, since the magnet 3 is made of expensive alnico material, there is also the disadvantage that the larger speaker becomes very expensive.
また、従来第3図示に示す如き外磁型磁気回路
を有するスピーカ11が提案されていた。この外
磁型磁気回路を有するスピーカ1では円柱状セン
ターポール12、一対のプレート4a,4b、磁
気ギヤツプ5、マグネツト3により磁気回路が構
成され、マグネツト3の着磁方向と同一方向にリ
ング状の磁気ギヤツプ5が形成されかかる同一方
向前後にスピーカ11の振動板7が振動し、所望
の音声を得る如くなされている。この外磁型磁気
回路を有するスピーカ11においてもギヤツプ内
磁束密度を高くしようとすれば、外磁マグネツト
3の内径方向にはマグネツトは伸ばせずマグネツ
ト3の外径を伸ばすしかないが、かかる外径が大
きくなると磁束利用率が低下してしまいその分を
補いつつ外径を大きくしなければならず第4図に
示すように磁気回路の幅方向及び奥行方向につい
ての大型化が必要となる。そのため、磁気回路の
幅あるいは奥行に寸法上の制約がある場合には所
望の十分なギヤツプ内磁束密度をもつた高品位の
外磁型磁気回路を有するスピーカ11を得ること
が出来ないという構造上の欠点があつた。また、
寸法の制約内で製造できるとしても外径増加によ
り磁気回路を構成している各部材の製造が高くつ
き、製品が高価となつてしまう欠点があつた。 Furthermore, a speaker 11 having an external magnet type magnetic circuit as shown in FIG. 3 has been proposed. In the speaker 1 having this external magnet type magnetic circuit, a magnetic circuit is constituted by a cylindrical center pole 12, a pair of plates 4a and 4b, a magnetic gap 5, and a magnet 3, and a ring-shaped magnetic circuit is formed in the same direction as the magnetization direction of the magnet 3. A magnetic gap 5 is formed so that the diaphragm 7 of the speaker 11 vibrates back and forth in the same direction to obtain desired sound. In order to increase the magnetic flux density in the gap in the speaker 11 having this outer magnetic type magnetic circuit, the magnet cannot be extended in the inner diameter direction of the outer magnet 3, and the only way is to extend the outer diameter of the magnet 3. When the magnetic flux becomes large, the magnetic flux utilization rate decreases, and the outer diameter must be increased while compensating for this, and as shown in FIG. 4, it is necessary to increase the size of the magnetic circuit in the width direction and the depth direction. Therefore, if there is a dimensional restriction on the width or depth of the magnetic circuit, it is structurally impossible to obtain a speaker 11 having a high-quality external magnet type magnetic circuit with a desired and sufficient in-gap magnetic flux density. There were some shortcomings. Also,
Even if it could be manufactured within the dimensional constraints, the increased outer diameter would make the manufacturing of each member constituting the magnetic circuit expensive, resulting in an expensive product.
本考案はかかる点に鑑み、寸法上の制約があつ
ても十分なギヤツプ5内磁束密度が得られるよう
にした動電型スピーカの磁気回路を提供せんとす
るものである。 In view of this, the present invention aims to provide a magnetic circuit for an electrodynamic speaker that can obtain a sufficient magnetic flux density within the gap 5 even if there are dimensional restrictions.
以下第5図及び第6図を参照して本考案スピー
カの一実施例について説明しよう。第5図及び第
6図において第1図及び第3図に対応する部分に
は同一符号を付しその詳細な説明は省略する。 Hereinafter, one embodiment of the speaker of the present invention will be described with reference to FIGS. 5 and 6. In FIGS. 5 and 6, parts corresponding to those in FIGS. 1 and 3 are designated by the same reference numerals, and detailed explanation thereof will be omitted.
第5図において、13は例えばアルニコ製の板
状マグネツトを示し着磁方向は第5図の上面側1
3aをN極、下面側13bをS極とし両平面に直
角な方向とする。14及び15は夫々例えば純鉄
製の別体形成する第1及び第2のヨークを示し、
これらのヨーク14及び15は夫々板状マグネツ
トの上・下平面の略全面を当接し、ヨーク14,
15で板状マグネツト13を挟んだ形のサンドイ
ツチ構造とする。また、16は例えば純鉄製のプ
レートを示し、このプレート16にはギヤツプ5
及びポールピース17用の円形孔を所定位置にマ
グネツト13の着磁方向と直角の方向に打ち抜い
て設ける様にし、磁気ギヤツプ5をマグネツト3
の着磁方向と直角の方向にリング状のものとして
形成する如くする。ここで、第6図に示すX軸方
向(幅)とY軸方向(奥行)の寸法は要求される
寸法制約に対応して設計段階に決定するものであ
る。尚、他の部分は従来のスピーカ同様に構成す
るものとする。 In FIG. 5, 13 indicates a plate-shaped magnet made of Alnico, for example, and the magnetization direction is on the top side 1 in FIG.
3a is the north pole, and the lower surface side 13b is the south pole in a direction perpendicular to both planes. 14 and 15 respectively indicate first and second yokes made of pure iron and formed separately;
These yokes 14 and 15 are in contact with substantially the entire upper and lower surfaces of the plate magnet, respectively.
It has a sandwich structure in which the plate magnet 13 is sandwiched between the magnets 15 and 15. Further, 16 indicates a plate made of pure iron, for example, and this plate 16 has a gap 5.
A circular hole for the pole piece 17 is punched out at a predetermined position in a direction perpendicular to the magnetization direction of the magnet 13, and the magnetic gap 5 is inserted into the magnet 3.
It is formed into a ring shape in a direction perpendicular to the direction of magnetization. Here, the dimensions in the X-axis direction (width) and Y-axis direction (depth) shown in FIG. 6 are determined at the design stage in accordance with required dimensional constraints. Note that the other parts are configured in the same manner as the conventional speaker.
また、スピーカの磁気回路について幅方向に寸
法制約を受けた場合に奥行を大きくもたせる様に
設計し所望の磁気ギヤツプ5内の磁束密度をもた
せたものとして第7図に示す如き磁気回路、スピ
ーカの磁気回路について奥行方向に寸法制約を受
けた場合に幅方向を広げて設計し所望の磁気ギヤ
ツプ5内の磁束密度をもたせたものとして第8図
に示す如き磁気回路を得ることができる。尚、こ
の第7図及び第8図において第5図に対応する部
分には同一符号を付しその詳細な説明は省略す
る。 Furthermore, when the magnetic circuit of a speaker is subject to dimensional constraints in the width direction, a magnetic circuit such as the one shown in FIG. When the magnetic circuit is subject to dimensional constraints in the depth direction, a magnetic circuit as shown in FIG. 8 can be obtained by widening the width in the width direction and providing a desired magnetic flux density within the magnetic gap 5. Note that in FIGS. 7 and 8, parts corresponding to those in FIG. 5 are designated by the same reference numerals, and detailed explanation thereof will be omitted.
このように構成された本実施例に依れば従来同
様所望の音声が得られると共に、磁気回路につい
てマグネツト13のX軸方向の長さ(幅)とY軸
方向の長さ(奥行)により決まる面積により所望
の磁束密度を得ることができるので寸法制約があ
つても必要とする磁気ギヤツプ5内高磁束密度を
もつた高品位のスピーカを得ることのできる利益
がある。また、磁束もれが極めて少なく磁束利用
率が高いのでかかるスピーカを安価に得ることの
できる利益がある。 According to this embodiment configured in this way, the desired sound can be obtained as in the conventional case, and the magnetic circuit is determined by the length (width) in the X-axis direction and the length (depth) in the Y-axis direction of the magnet 13. Since a desired magnetic flux density can be obtained depending on the area, there is an advantage that a high-quality speaker with a required high magnetic flux density within the magnetic gap 5 can be obtained even if there are dimensional restrictions. Further, since magnetic flux leakage is extremely small and magnetic flux utilization rate is high, there is an advantage that such a speaker can be obtained at a low cost.
また第9図は本考案の他の実施例の磁気回路部
分を示す。この第9図において第5図に対応する
部分には同一符号を付しその詳細な説明は省略す
る。この磁気回路は2点駆動のスピーカに本考案
を適用した場合の例であり、磁気ギヤツプ5を設
ける位置及び磁気ギヤツプ5を設ける個数の制約
の少ない本考案の特徴を活かして磁気ギヤツプ5
を2つ設ける様にしたものである。本例では、第
5図例同様の作用効果が得られることに加えて、
2点駆動型の小型スピーカを安価に得られる利益
がある。尚、この2点駆動型スピーカを2つ配し
て例えば第10図の如く応用すること、あるいは
ツイータ18及びウーハ19一体型ユニツトにし
て第11図の如く応用する実施例も可能である。 Further, FIG. 9 shows a magnetic circuit portion of another embodiment of the present invention. In FIG. 9, parts corresponding to those in FIG. 5 are given the same reference numerals, and detailed explanation thereof will be omitted. This magnetic circuit is an example in which the present invention is applied to a two-point drive speaker.
It is designed so that two are provided. In this example, in addition to obtaining the same effects as the example in FIG.
There is an advantage that a small two-point drive type speaker can be obtained at low cost. It is also possible to arrange two of these two-point drive type speakers and apply them, for example, as shown in FIG. 10, or to use an integrated unit of tweeter 18 and woofer 19 as shown in FIG. 11.
また、第12図は本考案の更に他の実施例を示
す。この第12図において第5図に対応する部分
には同一符号を付しその詳細な説明は省略する。
この第12図例は磁気回路部分が超スリムで振動
板が平板のスピーカに本考案を適用した例で第1
3図の如く磁気ギヤツプ5を4つ設けたものであ
る。本例においても上述実施例の作用効果が得ら
れることは容易に理解できよう。更に、板状マグ
ネツト13を円板状として第14図に示す如き無
指向性スピーカとする実施例も可能である。 Moreover, FIG. 12 shows still another embodiment of the present invention. In FIG. 12, parts corresponding to those in FIG. 5 are given the same reference numerals, and detailed explanation thereof will be omitted.
This example in Figure 12 is the first example in which the present invention is applied to a speaker with an ultra-slim magnetic circuit and a flat diaphragm.
As shown in Fig. 3, four magnetic gaps 5 are provided. It is easy to understand that the effects of the above-mentioned embodiments can also be obtained in this example. Furthermore, an embodiment in which the plate-shaped magnet 13 is made into a disc-shaped one to form an omnidirectional speaker as shown in FIG. 14 is also possible.
また、第1及び第2のヨーク14及び15、マ
グネツト13を一体でユニツト化すればプレート
16とポールピース17の変更のみで簡単に多岐
の寸法制約に対応できる利益もある。 Furthermore, if the first and second yokes 14 and 15 and the magnet 13 are integrated into a unit, there is the advantage that various dimensional constraints can be easily met by simply changing the plate 16 and the pole piece 17.
尚、本考案は上述実施例に限らず本考案の要旨
を逸脱しない範囲でその他種々の構成が取り得る
ことは勿論である。 It goes without saying that the present invention is not limited to the above-described embodiments, and that various other configurations may be adopted without departing from the gist of the present invention.
第1図及び第3図は従来のスピーカの例を示す
断面図、第2図及び第4図は夫々第1図例及び第
3図例の要部の例を示す断面図、第5図は本考案
動電型スピーカの磁気回路の一実施例を示す断面
図、第6図は本考案の一実施例の要部の例を示す
分解斜視図、第7図及び第8図は本考案の一実施
例の要部の例を示す斜視図、第9図は本考案の他
の実施例の要部の例を示す斜視図、第10図乃至
第12図は夫々本考案の他の実施例を示す正面
図、第13図は第12図例の要部の例を示す線
図、第14図は本考案の更に他の実施例を示す斜
視図である。
5は磁気ギヤツプ、6はボイスコイル、7は振
動板、13は板状マグネツト、14及び15は
夫々第1及び第2のヨーク、16はプレート、1
7はポールピースである。
1 and 3 are cross-sectional views showing examples of conventional speakers, FIGS. 2 and 4 are cross-sectional views showing main parts of the examples shown in FIGS. 1 and 3, respectively, and FIG. A sectional view showing an embodiment of the magnetic circuit of the electrodynamic speaker of the invention, FIG. 6 is an exploded perspective view showing an example of the main parts of an embodiment of the invention, and FIGS. FIG. 9 is a perspective view showing an example of the main part of one embodiment, FIG. 9 is a perspective view showing an example of the main part of another embodiment of the present invention, and FIGS. 10 to 12 are other embodiments of the present invention. FIG. 13 is a diagram showing an example of the essential parts of the example shown in FIG. 12, and FIG. 14 is a perspective view showing still another embodiment of the present invention. 5 is a magnetic gap, 6 is a voice coil, 7 is a diaphragm, 13 is a plate magnet, 14 and 15 are first and second yokes, respectively, 16 is a plate, 1
7 is the pole piece.
Claims (1)
トを挟持するように取り付けられると共に、上記
板状マグネツトの着磁方向の厚さが上記板状マグ
ネツトよりも小なる第1及び第2のヨークと、 該第1のヨークの上記板状マグネツトに当接す
る面と反対側の面に取り付けられたポールピース
と、 上記第2のヨークの一端に取り付けられると共
に、嵌挿される上記ポールピースとの間に上記板
状マグネツトの着磁方向と直角の方向にリング状
磁気ギヤツプが形成される円形孔を有するプレー
トとを備えたことを特徴とする動電型スピーカの
磁気回路。[Claims for Utility Model Registration] A plate-shaped magnet, which is attached to each magnetic pole face of the plate-shaped magnet so as to sandwich the plate-shaped magnet, and whose thickness in the magnetization direction is equal to the plate-shaped magnet. first and second yokes smaller than the magnet; a pole piece attached to a surface of the first yoke opposite to the surface that comes into contact with the plate magnet; and a pole piece attached to one end of the second yoke. and a plate having a circular hole in which a ring-shaped magnetic gap is formed in a direction perpendicular to the magnetization direction of the plate-shaped magnet between the plate and the pole piece to be inserted. Magnetic circuit of type speaker.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3823682U JPS58141691U (en) | 1982-03-18 | 1982-03-18 | Electrodynamic speaker magnetic circuit |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3823682U JPS58141691U (en) | 1982-03-18 | 1982-03-18 | Electrodynamic speaker magnetic circuit |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS58141691U JPS58141691U (en) | 1983-09-24 |
JPH0422637Y2 true JPH0422637Y2 (en) | 1992-05-25 |
Family
ID=30049590
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP3823682U Granted JPS58141691U (en) | 1982-03-18 | 1982-03-18 | Electrodynamic speaker magnetic circuit |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS58141691U (en) |
-
1982
- 1982-03-18 JP JP3823682U patent/JPS58141691U/en active Granted
Also Published As
Publication number | Publication date |
---|---|
JPS58141691U (en) | 1983-09-24 |
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