JPS5855732Y2 - magnetic circuit - Google Patents

magnetic circuit

Info

Publication number
JPS5855732Y2
JPS5855732Y2 JP13434379U JP13434379U JPS5855732Y2 JP S5855732 Y2 JPS5855732 Y2 JP S5855732Y2 JP 13434379 U JP13434379 U JP 13434379U JP 13434379 U JP13434379 U JP 13434379U JP S5855732 Y2 JPS5855732 Y2 JP S5855732Y2
Authority
JP
Japan
Prior art keywords
magnetic
magnets
magnet
magnetic circuit
magnetic flux
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
JP13434379U
Other languages
Japanese (ja)
Other versions
JPS5652391U (en
Inventor
保雄 海津
潔 斉藤
Original Assignee
日本ビクター株式会社
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 by 日本ビクター株式会社 filed Critical 日本ビクター株式会社
Priority to JP13434379U priority Critical patent/JPS5855732Y2/en
Publication of JPS5652391U publication Critical patent/JPS5652391U/ja
Application granted granted Critical
Publication of JPS5855732Y2 publication Critical patent/JPS5855732Y2/en
Expired legal-status Critical Current

Links

Description

【考案の詳細な説明】 本考案はリボン型スピーカ等に用いる磁気回路に係り、
従来のいわゆるプッシュプル型磁気回路よりも少ない数
の磁石にてこれと略同程度の磁束密度を得ることができ
る磁気回路を提供することを目的とする。
[Detailed description of the invention] The present invention relates to a magnetic circuit used in a ribbon type speaker, etc.
It is an object of the present invention to provide a magnetic circuit that can obtain approximately the same magnetic flux density with a smaller number of magnets than a conventional so-called push-pull type magnetic circuit.

ノボン型スピーカの磁気回路として用いる従来のシング
ル型磁気回路は、第1図A、Bに示す如く、ボイスコイ
ル1を設けられた膜面振動板2の片側にのみ磁石3を配
設した構成とされており、ボイスコイル1に音声信号に
応じた電流を流してフレミングの左手の法則によって膜
面振動板2を振動せしめ、発音せしめる。
A conventional single-type magnetic circuit used as a magnetic circuit for a Novon type speaker has a structure in which a magnet 3 is disposed only on one side of a membrane diaphragm 2 provided with a voice coil 1, as shown in FIGS. 1A and 1B. A current corresponding to the audio signal is passed through the voice coil 1 to cause the membrane diaphragm 2 to vibrate according to Fleming's left-hand rule, thereby producing sound.

然るに、このものは、磁石3が振動板2の片側にしか設
けられていないため、磁石3よりの磁束3′が磁気空隙
中に設けられたコイル1に集中しに<<、その周波数対
音圧特性は第2図の曲線1に示す如く、85dB〜88
dB程度の値しか得られず、能率が悪い欠点があった
However, in this case, since the magnet 3 is provided only on one side of the diaphragm 2, the magnetic flux 3' from the magnet 3 concentrates on the coil 1 provided in the magnetic gap, and the frequency As shown in curve 1 in Figure 2, the pressure characteristics range from 85 dB to 88 dB.
It had the disadvantage of being inefficient, as it could only obtain a value of about dB.

そこでこの改良型として従来あるプッシュプル型磁気回
路は、第3図に示す如く、振動板2の両側に磁石3a、
3bを同性の磁極面どうし対向配設した構成とされてい
る。
Therefore, the conventional push-pull magnetic circuit as an improved version has magnets 3a on both sides of the diaphragm 2, as shown in FIG.
3b are arranged so that the magnetic pole faces of the same sex are opposed to each other.

このものは、磁石3a、3bによる磁束3 a’、3
b’がコイル1に集中するために第1図A、Bに示すも
のよりも良好な周波数特性を得ることができるが、磁石
の数が多く、軽量かつ安価に構成し得ない欠点があった
This thing has magnetic fluxes 3a', 3 due to magnets 3a, 3b.
Since b' is concentrated in coil 1, it is possible to obtain better frequency characteristics than those shown in Fig. 1 A and B, but it has the disadvantage that it requires a large number of magnets and cannot be constructed lightweight and inexpensively. .

本考案は上記欠点を除去したものであり、第4図以下と
共にその一実施例について説明する。
The present invention eliminates the above-mentioned drawbacks, and one embodiment thereof will be described with reference to FIG. 4 and the following figures.

第4図は本考案になる磁気回路の一実施例の概略構成図
を示し、第1図A、Bと同一構成部分には同一番号を付
す。
FIG. 4 shows a schematic diagram of an embodiment of the magnetic circuit according to the present invention, and the same components as those in FIGS. 1A and 1B are given the same numbers.

同図において、磁石3、は磁極S、磁石32は磁極N、
磁石33は磁極Sを夫々振動板2に対向するようにヨー
ク4に並設されている。
In the same figure, the magnet 3 is a magnetic pole S, the magnet 32 is a magnetic pole N,
The magnets 33 are arranged in parallel to the yoke 4 so that their magnetic poles S face the diaphragm 2.

一方、磁石5は中央の磁石32と対向する位置に振動板
2を介して磁石3□と同性の磁極面どうし対向させてヨ
ーク6に固定されている。
On the other hand, the magnet 5 is fixed to the yoke 6 at a position facing the central magnet 32 with the diaphragm 2 in between, with the magnetic pole faces of the same sex as the magnet 3□ facing each other.

このように構成すれば、磁極3□のN極よりの磁束3□
′は磁石30,33のS極に至る一方、磁石5のN極よ
りの磁束5′は磁石3□、33のS極に至り、磁束32
′は磁束5′によって図中上方向へ漏洩することはない
With this configuration, the magnetic flux 3□ from the N pole of the magnetic pole 3□
' reaches the south pole of magnets 30, 33, while the magnetic flux 5' from the north pole of magnet 5 reaches the south pole of magnets 3□, 33, and the magnetic flux 32
' does not leak upward in the figure due to the magnetic flux 5'.

これにより、第1図A、Bに示す従来のものよりもコイ
ル1に磁束が集中し易く、その周波数対音圧特性は第2
図の曲線IIに示す如く、87dA〜93 dB程度の
値を得ることができる。
As a result, magnetic flux is more easily concentrated in the coil 1 than in the conventional ones shown in Fig. 1A and B, and its frequency vs. sound pressure characteristics are second to none.
As shown by curve II in the figure, a value of about 87 dA to 93 dB can be obtained.

又、磁束5′は外部へ漏洩することなく磁石3i、3a
に至るため、磁石5,3□と磁石3、と9間、磁石5,
3□と磁石33との間の磁気空隙における磁束密度は第
3図に示す従来のプッシュプル型磁気回路のものと略同
程度得ることができ、このものと略同程度の音圧を得る
ことができ、しかも、このものよりも磁石を少なく構威
し得、軽量かつ安価に構成し得る。
Moreover, the magnetic flux 5' is connected to the magnets 3i and 3a without leaking to the outside.
To reach this, between magnets 5, 3□ and magnets 3 and 9, magnets 5,
The magnetic flux density in the magnetic air gap between 3□ and the magnet 33 can be obtained to be approximately the same as that of the conventional push-pull type magnetic circuit shown in FIG. Moreover, it can be constructed with fewer magnets than this one, and can be constructed lightweight and inexpensively.

第5図は本考案回路の他の実施例の概略図を示し、第4
図は同一構成部分には同一番号を付す。
FIG. 5 shows a schematic diagram of another embodiment of the circuit of the present invention;
In the figures, the same components are given the same numbers.

このものは、3個所の磁気空隙にコイル7を配設したも
のであり、磁石3..33はS極、磁石32,34はN
極を夫々振動板2に対向するように設けられており、磁
石51は磁石30、磁石5□は磁石3□に夫々同性の磁
極面どうし対向するように設けられている。
This device has coils 7 arranged in three magnetic gaps, with magnets 3. .. 33 is an S pole, and magnets 32 and 34 are N poles.
The magnets 51 and 5□ and the magnet 5□ and 3□, respectively, are provided so that their poles face the diaphragm 2, and the magnetic pole faces of the same sex face each other.

このものも、シングル型の磁気回路に比して磁束がコイ
ル7に集中し易く、又、振動板の両側に同数の磁石を配
設したプッシュプル型の磁気回路に比して軽量かつ安価
に構成し得る。
This also makes it easier for magnetic flux to concentrate on the coil 7 compared to a single type magnetic circuit, and is lighter and cheaper than a push-pull type magnetic circuit in which the same number of magnets are arranged on both sides of the diaphragm. Can be configured.

第6図は本考案回路の更に他の実施例の概略図を示す。FIG. 6 shows a schematic diagram of yet another embodiment of the circuit of the present invention.

このものは、4個所の磁気空隙にコイル8を配設したも
のであり、第4図及び第5図に示す実施例より容易に理
解し得るため、その説明を省略する。
This device has coils 8 disposed in four magnetic gaps, and since it can be more easily understood than the embodiment shown in FIGS. 4 and 5, the explanation thereof will be omitted.

上述の如く、本考案になる磁気回路は、平面状に並設さ
れた複数の第1の磁石のうち端部にある磁石を除いた磁
石にその磁極と同性の磁極を対向させて第2の磁石を配
設したため、従来のシングル型磁気回路に比して磁気空
隙に磁束を集中せしめ易く、これにより、従来のシング
ル型磁気回路よりも大なる音圧を得ることができ、又、
従来のプッシュプル型磁気回路のように第1の磁石全て
に対して第2の磁石を配設しているのではないため、こ
のものよりも磁石を少なく構成し得、軽量かつ安価に構
成し得、しかも、磁束は外部へ殆ど漏洩することはない
ため、磁気空隙における磁束密度は従来のプッシュプル
型磁気回路のそれと略同程度得ることができ、これと略
同程度の音圧を得ることができる等の特長を有する。
As described above, the magnetic circuit according to the present invention includes a plurality of first magnets arranged in parallel in a plane, excluding the magnets at the ends, with magnetic poles of the same sex as those of the first magnets facing each other, and a second magnet. Because the magnet is provided, it is easier to concentrate magnetic flux in the magnetic gap than in a conventional single-type magnetic circuit, and as a result, it is possible to obtain a higher sound pressure than in a conventional single-type magnetic circuit.
Unlike conventional push-pull type magnetic circuits, the second magnet is not arranged for all the first magnets, so it can be configured with fewer magnets than this one, making it lighter and cheaper. Furthermore, since almost no magnetic flux leaks to the outside, the magnetic flux density in the magnetic air gap can be obtained to be approximately the same as that of a conventional push-pull type magnetic circuit, and approximately the same level of sound pressure can be obtained. It has features such as being able to

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

第1図A、Bは夫々従来のシングル型磁気回路の一例を
概略正面図及び概略斜視図、第2図は第1図A、Bに示
す従来の磁気回路及び本考案になる磁気回路をリボン型
スピーカに適用した際の周波数対音圧特性図、第3図は
従来のプッシュプル型磁気回路の一例の概略正面図、第
4図乃至第6図は本考案になる磁気回路の各実施例の概
略正面図である。 1.7.8・・・・・・ボイスコイル、2・・・・・・
膜面振動板、3、〜3.,5,5.〜53・・・・・・
磁石、32′、5′・・・・・・磁束、4,6・・・・
・・ヨーク。
1A and 1B are schematic front views and schematic perspective views of an example of a conventional single-type magnetic circuit, respectively, and FIG. 2 is a ribbon illustrating the conventional magnetic circuit shown in FIGS. Figure 3 is a schematic front view of an example of a conventional push-pull type magnetic circuit, and Figures 4 to 6 are examples of the magnetic circuit according to the present invention. FIG. 1.7.8...Voice coil, 2...
Membrane diaphragm, 3, ~3. ,5,5. ~53...
Magnet, 32', 5'...Magnetic flux, 4,6...
··yoke.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 複数の第1の磁石を平面状にその磁極面を該平面と直角
方向に向けて磁気空隙を以て並設すると共に、第2の磁
石を該平面と直角方向上に該第1の磁石と磁気空隙を以
て該第1の磁石の磁極と同性の磁極を対向させて配設し
てなる磁気回路において、上記複数個の第1の磁石のう
ち端部にある磁石を除いた磁石に上記第2の磁石を対向
配設してなる磁気回路。
A plurality of first magnets are arranged side by side in a plane with their magnetic pole faces perpendicular to the plane with a magnetic gap between them, and a second magnet is arranged in a direction perpendicular to the plane with a magnetic gap between them and the first magnets. In a magnetic circuit in which magnetic poles of the same sex as the magnetic poles of the first magnet are arranged to face each other, the second magnet is attached to the plurality of first magnets excluding the magnet at the end. A magnetic circuit formed by arranging them facing each other.
JP13434379U 1979-09-28 1979-09-28 magnetic circuit Expired JPS5855732Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13434379U JPS5855732Y2 (en) 1979-09-28 1979-09-28 magnetic circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13434379U JPS5855732Y2 (en) 1979-09-28 1979-09-28 magnetic circuit

Publications (2)

Publication Number Publication Date
JPS5652391U JPS5652391U (en) 1981-05-08
JPS5855732Y2 true JPS5855732Y2 (en) 1983-12-21

Family

ID=29365914

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13434379U Expired JPS5855732Y2 (en) 1979-09-28 1979-09-28 magnetic circuit

Country Status (1)

Country Link
JP (1) JPS5855732Y2 (en)

Also Published As

Publication number Publication date
JPS5652391U (en) 1981-05-08

Similar Documents

Publication Publication Date Title
US3919498A (en) Electroacoustic transducer
JP2009278523A (en) Speaker
US4295011A (en) Linear excursion-constant inductance loudspeaker
JPS5855732Y2 (en) magnetic circuit
JPH08317489A (en) Speaker device
JPS6028400A (en) Dynamic speaker
JPH06233384A (en) Speaker
US2494918A (en) Inductively energized electro-dynamic loud-speaker
US2927977A (en) Acoustic signal transducers
JPH0623115Y2 (en) Flat speaker
US3584161A (en) Balanced magnetic transducer
JPH0424715Y2 (en)
JPS589438Y2 (en) magnetic circuit
JPS5955699A (en) Entirely dynamic driving speaker
GB803283A (en) Improvements in or relating to electroacoustic transducers
WO2021128087A1 (en) Speaker unit
JPS5931110Y2 (en) electrodynamic speaker
JPH0221839Y2 (en)
JPS5855735Y2 (en) Speaker unit using square planar diaphragm
JPS61255199A (en) Low magnetic leakage speaker system
JPS6035360Y2 (en) Moving coil type pick-up cartridge
JP4514947B2 (en) Speaker
JPH0422638Y2 (en)
JPH046319Y2 (en)
JPH09154193A (en) Speaker for preventing leakage magnetic flux