JPH09163495A - Linear voice coil for dual gap - Google Patents

Linear voice coil for dual gap

Info

Publication number
JPH09163495A
JPH09163495A JP34731595A JP34731595A JPH09163495A JP H09163495 A JPH09163495 A JP H09163495A JP 34731595 A JP34731595 A JP 34731595A JP 34731595 A JP34731595 A JP 34731595A JP H09163495 A JPH09163495 A JP H09163495A
Authority
JP
Japan
Prior art keywords
voice coil
gap
magnetic
winding width
dual
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
Application number
JP34731595A
Other languages
Japanese (ja)
Other versions
JP3598423B2 (en
Inventor
Hidetoshi Shirakawa
英俊 白川
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Foster Electric Co Ltd
Original Assignee
Foster Electric Co Ltd
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 Foster Electric Co Ltd filed Critical Foster Electric Co Ltd
Priority to JP34731595A priority Critical patent/JP3598423B2/en
Publication of JPH09163495A publication Critical patent/JPH09163495A/en
Application granted granted Critical
Publication of JP3598423B2 publication Critical patent/JP3598423B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Abstract

PROBLEM TO BE SOLVED: To keep driving power constant regardlessly of amplitude of voice coil and to improve the efficiency of driving power. SOLUTION: A linear voice coil 7 for dual gap is inserted and arranged in a gap 5 of dual gap magnetic circuit composed of magnet 1, top plate 2 having plate thickness Tp, bottom plate 3 having plate thickness Tp and yoke 4. Winding width Lc of upper voice coil 7a and lower voice coil 7b is made equal with or less than the plate thickness Tp and winding directions are inverted each other. The total of lower section of upper voice coil 7a inside an upper magnetic gap 5a and the upper section of lower voice coil 7b inside a lower magnetic gap 5b is made equal with the winding width Lc. Thus, the total winding width of voice coils inside two magnetic gaps 5a and 5b is fixed rehardlessly of amplitude, the driving power of linear voice coil 7 for dual gap is not fluctuated, and efficiency is more improved.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【発明の属する技術分野】本発明は電気音響変換器に使
用されるボイスコイルに関し、特に振幅による出力変動
のないデュアルギャップ用リニアボイスコイルに関す
る。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a voice coil used in an electroacoustic transducer, and more particularly to a dual-gap linear voice coil having no output fluctuation due to amplitude.

【0002】[0002]

【従来の技術】図2は従来例1における磁気回路とボイ
スコイルの半断面図である。図において、1はマグネッ
トであり、2はこのマグネツト1の上部に設置された板
厚Tpのトッププレートであり、14はマグネツト1の
下部と外周に位置するヨークであり、15はトッププレ
ート2とヨーク14間の磁気ギャップである。17はこ
の磁気ギャップ15内に挿入配置されるボイスコイルで
あり、このボイスコイル17の巻巾Lcはトッププレー
ト2の板厚Tpと略同じか少し小さめである。
2. Description of the Related Art FIG. 2 is a half sectional view of a magnetic circuit and a voice coil in a first conventional example. In the figure, 1 is a magnet, 2 is a top plate having a plate thickness Tp installed on the upper part of the magnet 1, 14 is a yoke located at the lower part and outer periphery of the magnet 1, and 15 is a top plate 2. It is a magnetic gap between the yokes 14. Reference numeral 17 denotes a voice coil inserted and arranged in the magnetic gap 15. The winding width Lc of the voice coil 17 is substantially the same as or slightly smaller than the plate thickness Tp of the top plate 2.

【0003】マグネツト1で発生する磁束はトッププレ
ート2→磁気ギャップ15→ヨーク14→マグネツト1
と1巡し、磁気回路を構成している。ここで、ボイスコ
イル17に電流を流すとフレミングの法則に従って電流
の向きにより上下方向に駆動する。ここで、磁気ギャッ
プ15における磁束をbとすると、磁気ギャップ15内
に挿入されているボイスコイル17の巻巾はLcである
から、ボイスコイル17の駆動力はb・Lcに比例す
る。
The magnetic flux generated in the magnet 1 is the top plate 2 → the magnetic gap 15 → the yoke 14 → the magnet 1
The magnetic circuit is formed by making one round. Here, when a current is passed through the voice coil 17, the voice coil 17 is driven vertically according to the direction of the current according to Fleming's law. Here, when the magnetic flux in the magnetic gap 15 is b, the winding width of the voice coil 17 inserted in the magnetic gap 15 is Lc, so the driving force of the voice coil 17 is proportional to b · Lc.

【0004】この従来例1は有効に磁束を利用している
が、ボイスコイル17の振幅により駆動力は変動し、磁
気ギャップ15における磁束密度分布が上下方向に非対
称なために、磁気ギャップ15内に挿入配置したボイス
コイル17は上方に移行する場合と下方に移行する場合
とでその動作が異なり、スピーカの低域における第2調
波歪を発生させていた。又、このボイスコイル17では
高域でのインピーダンスが上昇し、スピーカの高域特性
に悪影響を与えていた。
In the prior art example 1, the magnetic flux is effectively utilized. However, the driving force fluctuates depending on the amplitude of the voice coil 17, and the magnetic flux density distribution in the magnetic gap 15 is asymmetric in the vertical direction. The operation of the voice coil 17 inserted and arranged differently depending on whether it moves upward or downward, causing second harmonic distortion in the low range of the speaker. Further, the impedance of the voice coil 17 in the high frequency range is increased, which adversely affects the high frequency characteristics of the speaker.

【0005】図3は従来例1の上記欠点を改善した従来
例2における磁気回路とボイスコイルの半断面図であ
る。図において、1は従来例1と同じマグネットであ
り、2はこのマグネツト1の上部に設置された従来例1
と同じトッププレートであり、14はマグネツト1の下
部と外周に位置する従来例1と同じヨークであり、15
はトッププレート2とヨーク14間の磁気ギャップであ
る。27はこの磁気ギャップ15に挿入配置される上部
ボイスコイル27aと下部ボイスコイル27bから成る
ボイスコイルであり、これらの上部ボイスコイル27a
と下部ボイスコイル27bの巻巾は従来例1のボイスコ
イル17の半分のLc/2で、トッププレート2の板厚
Tpの略半分である。但し、上部ボイスコイル27aと
下部ボイスコイル27bとは互いに巻き方向が逆であ
り、互いに接続されている。磁気ギャップ15内に挿入
されている上部ボイスコイル27aの下部部分と下部ボ
イスコイル27bの上部部分との合計はLc/2となっ
ている。
FIG. 3 is a half sectional view of a magnetic circuit and a voice coil in Conventional Example 2 in which the above-mentioned drawbacks of Conventional Example 1 are improved. In the figure, 1 is the same magnet as the conventional example 1, and 2 is the conventional example 1 installed above the magnet 1.
14 is the same yoke as in the conventional example 1 located on the lower and outer circumferences of the magnet 1,
Is a magnetic gap between the top plate 2 and the yoke 14. Reference numeral 27 denotes a voice coil composed of an upper voice coil 27a and a lower voice coil 27b which are inserted and arranged in the magnetic gap 15, and these upper voice coils 27a.
The winding width of the lower voice coil 27b is Lc / 2, which is half that of the voice coil 17 of Conventional Example 1, and is approximately half the plate thickness Tp of the top plate 2. However, the upper voice coil 27a and the lower voice coil 27b have opposite winding directions and are connected to each other. The total of the lower portion of the upper voice coil 27a and the upper portion of the lower voice coil 27b inserted in the magnetic gap 15 is Lc / 2.

【0006】マグネツト1で発生する磁束はトッププレ
ート2→磁気ギャップ15→ヨーク14→マグネツト1
と1巡し、磁気回路を構成している。ここで、上部ボイ
スコイル27aと下部ボイスコイル27bとに電流を流
すとフレミングの法則に従って電流の向きにより上下方
向に駆動し、振幅の如何に係わらず磁気ギャップ15内
のボイスコイルの巻巾の合計はLc/2と一定であり、
ボイスコイル27の駆動力の変動はない。ここで、磁気
ギャップ15における磁束をbとすると、磁気ギャップ
15内に挿入されているボイスコイル27の巻巾の合計
はLc/2であるから、ボイスコイル27の駆動力は
0.5b・Lcに比例し、一定となる。
The magnetic flux generated in the magnet 1 is the top plate 2 → the magnetic gap 15 → the yoke 14 → the magnet 1
The magnetic circuit is formed by making one round. Here, when a current is passed through the upper voice coil 27a and the lower voice coil 27b, the voice coil is driven in the vertical direction according to the direction of the current according to Fleming's law, and the total winding width of the voice coil in the magnetic gap 15 regardless of the amplitude. Is constant at Lc / 2,
There is no change in the driving force of the voice coil 27. Here, assuming that the magnetic flux in the magnetic gap 15 is b, the total winding width of the voice coil 27 inserted in the magnetic gap 15 is Lc / 2, so the driving force of the voice coil 27 is 0.5b · Lc. Is proportional to and becomes constant.

【0007】[0007]

【発明が解決しようとする課題】しかし、従来例2の1
つの磁気ギャップに上部と下部の2つのボイスコイルか
らなるボイスコイルでは1つの磁気ギャップに1つのボ
イスコイルを使用している場合に比べて駆動力が1/2
となり効率が悪い。
However, 1 of the conventional example 2
A voice coil consisting of two voice coils, an upper voice coil and a lower voice coil in one magnetic gap, has half the driving force compared to the case where one voice coil is used in one magnetic gap.
Becomes less efficient.

【0008】本発明はこのような点に鑑みてなされたも
のであり、振幅に係わらず駆動力は変動せず、かつ、効
率を向上させたデュアルギャップ用リニアボイスコイル
を提供することを目的とする。
The present invention has been made in view of the above circumstances, and an object thereof is to provide a linear voice coil for a dual gap in which the driving force does not change regardless of the amplitude and the efficiency is improved. To do.

【0009】[0009]

【課題を解決するための手段】上記課題を解決するため
に本発明のデュアルギャップ用リニアボイスコイルは、
互いに巻き方向が逆でトッププレートの板厚と同じかよ
り小さい巻巾の上部ボイスコイルと下部ボイスコイルの
2つのボイスコイルから成り、デュアルギャップ磁気回
路の互いに磁束方向が逆である2つの磁気ギャップ内に
挿入配置するものである。上部磁気ギャップ内に挿入さ
れている上部ボイスコイルの下部部分と下部磁気ギャッ
プ内に挿入されている下部ボイスコイルの上部部分との
巻巾が同じで、かつ、合計が一方のボイスコイルの巻巾
と等しくすることによって、デュアルギャップ用リニア
ボイスコイルの駆動力は変動はなく、かつ、効率が一段
と向上する。
In order to solve the above problems, the dual gap linear voice coil of the present invention is
Two magnetic gaps, which have opposite voice directions and two voice coils, an upper voice coil and a lower voice coil, whose winding width is equal to or smaller than the thickness of the top plate, and the magnetic flux directions of the dual gap magnetic circuits are opposite to each other. It is to be inserted and placed inside. The lower part of the upper voice coil inserted in the upper magnetic gap and the upper part of the lower voice coil inserted in the lower magnetic gap have the same winding width, and the total winding width of one voice coil is By making them equal to, the driving force of the dual-gap linear voice coil does not fluctuate, and the efficiency is further improved.

【0010】[0010]

【発明の実施の形態】本発明のデュアルギャップ用リニ
アボイスコイルは、マグネット1の上部と下部に板厚が
同じであるトッププレート2とボトムプレート3を各々
設置し、これらの外周にヨーク4を設置して上部磁気ギ
ャップ5aと下部磁気ギャップ5bを有するギャップ5
を形成するデュアルギャップ磁気回路を設け、このギャ
ップ5内に挿入配置されるデュアルギャップ用リニアボ
イスコイル7において、互いに接続されており、同じ巻
巾で巻き方向が逆である上部ボイスコイル7aと下部ボ
イスコイル7bからなり、巻巾がトッププレート2の板
厚と同じかより小さく、上部磁気ギャップ5a内に挿入
されている上部ボイスコイル7aの下部部分と下部磁気
ギャップ5b内に挿入されている下部ボイスコイル7b
の上部部分との巻巾が同じで、かつ、合計が一方のボイ
スコイルの巻巾と同じであることに特徴を有している。
BEST MODE FOR CARRYING OUT THE INVENTION The dual-gap linear voice coil of the present invention is provided with a top plate 2 and a bottom plate 3 having the same plate thickness on the upper and lower parts of a magnet 1, respectively, and a yoke 4 on the outer periphery thereof. The gap 5 which is installed and has an upper magnetic gap 5a and a lower magnetic gap 5b
A dual-gap magnetic circuit for forming a dual-gap linear voice coil 7 that is inserted into the gap 5 and is connected to each other in the dual-gap linear voice coil 7. The lower part of the upper voice coil 7a, which is composed of the voice coil 7b and has a winding width equal to or smaller than the plate thickness of the top plate 2, is inserted into the upper magnetic gap 5a and the lower part is inserted into the lower magnetic gap 5b. Voice coil 7b
Is characterized in that the winding width is the same as that of the upper part and the total width is the same as the winding width of one voice coil.

【0011】[0011]

【実施例】以下、本発明の一実施例を図面に基づいて説
明する。図1はデュアルギャップ磁気回路と本発明によ
るデュアルギャップ用リニアボイスコイルの半断面図で
ある。図において、1は従来例と同じマグネットであ
り、2はこのマグネツト1の上部に設置された従来例と
同じトッププレートであり、3はこのマグネツト1の下
部に設置された板厚Tpのボトムプレートである。4は
マグネツト1,トッププレート2,ボトムプレート3の
外周に設置されたヨークであり、5aはトッププレート
2とヨーク4間の上部磁気ギャップであり、5bはボト
ムプレート3とヨーク4間の下部磁気ギャップであり、
5はこれらの上部磁気ギャップ5aと下部磁気ギャップ
5bを有するギャップである。
An embodiment of the present invention will be described below with reference to the drawings. FIG. 1 is a half sectional view of a dual gap magnetic circuit and a dual gap linear voice coil according to the present invention. In the figure, 1 is the same magnet as the conventional example, 2 is the same top plate as the conventional example installed on the upper part of the magnet 1, and 3 is a bottom plate with a plate thickness Tp installed at the lower part of the magnet 1. Is. Reference numeral 4 is a yoke installed on the outer periphery of the magnet 1, top plate 2 and bottom plate 3, 5a is an upper magnetic gap between the top plate 2 and the yoke 4, and 5b is a lower magnetic gap between the bottom plate 3 and the yoke 4. Is a gap,
Reference numeral 5 is a gap having the upper magnetic gap 5a and the lower magnetic gap 5b.

【0012】7はギャップ5に挿入配置される上部ボイ
スコイル7aと下部ボイスコイル7bから成るデュアル
ギャップ用リニアボイスコイルであり、これらの上部ボ
イスコイル7aと下部ボイスコイル7bの巻巾Lcはト
ッププレート2の板厚Tpと同じかより小さいが、板厚
Tpと略同じであることが望ましい。但し、上部ボイス
コイル7aと下部ボイスコイル7bは互いに巻き方向が
逆であり、互いに接続されている。
Reference numeral 7 is a dual-gap linear voice coil consisting of an upper voice coil 7a and a lower voice coil 7b inserted in the gap 5, and the winding width Lc of the upper voice coil 7a and the lower voice coil 7b is a top plate. Although it is equal to or smaller than the plate thickness Tp of No. 2, it is desirable that it is substantially the same as the plate thickness Tp. However, the upper voice coil 7a and the lower voice coil 7b have winding directions opposite to each other and are connected to each other.

【0013】マグネツト1で発生する磁束はトッププレ
ート2→上部磁気ギャップ5a→ヨーク4→下部磁気ギ
ャップ5b→マグネツト1と1巡し、磁気回路を構成し
ている。ここで、上部ボイスコイル7aと下部ボイスコ
イル7bとに電流を流すとフレミングの法則に従って電
流の向きにより上下方向に駆動する。上部磁気ギャップ
5a内に挿入されている上部ボイスコイル7aの下部部
分と下部磁気ギャップ5b内に挿入されている下部ボイ
スコイル7bの上部部分との巻巾が同じで、かつ、合計
が一方のボイスコイルの巻巾と等しくするにより、振幅
の如何に係わらず2つの磁気ギャップ5a,5b内のボ
イスコイルの巻巾の合計はLcと一定であり、デュアル
ギャップ用リニアボイスコイル7の駆動力の変動はな
く、かつ、効率が一段と向上する。
The magnetic flux generated in the magnet 1 makes one circuit in the order of top plate 2 → upper magnetic gap 5a → yoke 4 → lower magnetic gap 5b → magnet 1 to form a magnetic circuit. Here, when a current is passed through the upper voice coil 7a and the lower voice coil 7b, the current is driven in the vertical direction according to the direction of the current according to Fleming's law. A voice having the same winding width between the lower part of the upper voice coil 7a inserted in the upper magnetic gap 5a and the upper part of the lower voice coil 7b inserted in the lower magnetic gap 5b, and having a total of one voice By making the winding width of the coil equal, the total winding width of the voice coils in the two magnetic gaps 5a and 5b is constant as Lc regardless of the amplitude, and the driving force of the dual gap linear voice coil 7 varies. Moreover, the efficiency is further improved.

【0014】図1における実施例では、従来例1,2と
の比較のために、マグネット,トッププレートは従来例
の物と同じであり、ボイスコイルの巻巾の単位も等しく
してある。実施例では磁気ギャップが2つであり、その
分従来例に比して磁束密度が減少している。ここでは、
上部磁気ギャップ5aと下部磁気ギャップ5bにおける
磁束を従来例における磁気ギャップ15の0.9とし、
上部ボイスコイル7aと下部ボイスコイル7bの各巻線
の全長を短くすることによって実効巻巾を0.8として
いる。従って、磁気ギャップ5a,5bにおける磁束は
0.9bとなり、磁気ギャップ5a,5b内に挿入され
ている上部ボイスコイル7a,下部ボイスコイル7bの
巻巾の合計は0.8Lcとなるので、デュアルギャップ
用リニアボイスコイル7の駆動力は0.72b・Lcに
比例し、一定となる。
In the embodiment shown in FIG. 1, for comparison with the conventional examples 1 and 2, the magnet and the top plate are the same as those of the conventional example, and the unit of the winding width of the voice coil is also the same. In the embodiment, there are two magnetic gaps, and the magnetic flux density is reduced by that amount as compared with the conventional example. here,
The magnetic flux in the upper magnetic gap 5a and the lower magnetic gap 5b is set to 0.9 of the magnetic gap 15 in the conventional example,
The effective winding width is set to 0.8 by shortening the total length of each winding of the upper voice coil 7a and the lower voice coil 7b. Therefore, the magnetic flux in the magnetic gaps 5a and 5b is 0.9b, and the total winding width of the upper voice coil 7a and the lower voice coil 7b inserted in the magnetic gaps 5a and 5b is 0.8Lc. The driving force of the linear voice coil 7 for use is constant in proportion to 0.72b · Lc.

【0015】従来例1(図2参照)の磁気ギャップが1
つ、ボイスコイルの巻線部が1つの場合にはボイスコイ
ルの駆動力は磁束bとコイル巻巾Lcとの積、すなわ
ち、b・Lcに比例する。従来例2(図3参照)の磁気
ギャップが1つ、ボイスコイルの巻線部が2つの場合に
はボイスコイルの駆動力は磁束bと有効なコイル巻巾の
合計Lc/2との積、すなわち、0.5b・Lcに比例
し、一定となる。本発明の実施例(図1参照)における
磁気ギャップが2つ、ボイスコイルの巻線部が2の場合
にはボイスコイルの駆動力は磁束0.9bと有効なコイ
ル巻巾の合計0.8Lcとの積、すなわち、0.72b
・Lcに比例し、一定となり、従来例に比べて効率が良
くなる。
In the conventional example 1 (see FIG. 2), the magnetic gap is 1
On the other hand, when the voice coil has one winding portion, the driving force of the voice coil is proportional to the product of the magnetic flux b and the coil winding width Lc, that is, b · Lc. In the case of the conventional example 2 (see FIG. 3) having one magnetic gap and two voice coil winding portions, the driving force of the voice coil is the product of the magnetic flux b and the total effective coil winding width Lc / 2. That is, it is constant in proportion to 0.5b · Lc. In the embodiment of the present invention (see FIG. 1), when there are two magnetic gaps and the voice coil has two winding portions, the driving force of the voice coil is a total of 0.8Lc of the magnetic flux 0.9b and the effective coil winding width. Product with, that is, 0.72b
・ Proportion to Lc, which is constant and is more efficient than the conventional example.

【0016】[0016]

【発明の効果】本発明のデュアルギャップ用リニアボイ
スコイルは、互いに接続されており、同じ巻巾で巻き方
向が逆である上部ボイスコイル7aと下部ボイスコイル
7bからなり、巻巾がトッププレート2の板厚と同じか
より小さく、上部磁気ギャップ5a内に挿入されている
上部ボイスコイル7aの下部部分と下部磁気ギャップ5
b内に挿入されている下部ボイスコイル7bの上部部分
との巻巾が同じで、かつ、合計が一方のボイスコイルの
巻巾と同じであるので、デュアルギャップ用リニアボイ
スコイル7が振幅しても駆動力を一定にでき、上部ボイ
スコイル7aに流れる電流と下部ボイスコイル7bに流
れる電流とが逆向きとなるためにインダクタンスを相互
に打消すことで高い周波数でのインピーダンスの上昇を
おさえることができ、高域特性改善又電流歪を減少させ
る効果がある。また、1つの磁気ギャップに2つの巻線
部を持つコイルを設置した従来例に比べて、本発明は2
つの磁気ギャップに2つの巻線部を各々に1つづつ設置
したために効率が良い。
The dual-gap linear voice coil of the present invention is composed of an upper voice coil 7a and a lower voice coil 7b which are connected to each other and have the same winding width but opposite winding directions. And the lower magnetic gap 5 which is equal to or smaller than the plate thickness of the upper voice coil 7a inserted in the upper magnetic gap 5a.
Since the winding width of the upper part of the lower voice coil 7b inserted in b is the same, and the total is the same as the winding width of one voice coil, the linear voice coil 7 for dual gap is oscillated. The driving force can be made constant, and the current flowing through the upper voice coil 7a and the current flowing through the lower voice coil 7b are in opposite directions, so that the inductances can be canceled out from each other, thereby suppressing the increase in impedance at high frequencies. This has the effect of improving high frequency characteristics and reducing current distortion. Further, compared with the conventional example in which a coil having two winding portions is installed in one magnetic gap, the present invention has two
It is efficient because two winding parts are installed in each magnetic gap.

【図面の簡単な説明】[Brief description of the drawings]

【図1】デュアルギャップ磁気回路と本発明によるデュ
アルギャップ用リニアボイスコイルの半断面図である。
FIG. 1 is a half sectional view of a dual gap magnetic circuit and a dual gap linear voice coil according to the present invention.

【図2】従来例1における磁気回路とボイスコイルの半
断面図である。
FIG. 2 is a half cross-sectional view of a magnetic circuit and a voice coil in Conventional Example 1.

【図3】従来例2における磁気回路とボイスコイルの半
断面図である。
FIG. 3 is a half sectional view of a magnetic circuit and a voice coil in Conventional Example 2.

【符号の説明】[Explanation of symbols]

1 マグネット 2 トッププレート 3 ボトムプレート 4,14 ヨーク 5,15 ギャップ 5a 上部磁気ギャップ 5b 下部磁気ギャップ 7 デュアルギャップ用リニアボイスコイル 7a,27a 上部ボイスコイル 7b,27b 下部ボイスコイル 17,27 ボイスコイル 1 magnet 2 top plate 3 bottom plate 4,14 yoke 5,15 gap 5a upper magnetic gap 5b lower magnetic gap 7 dual gap linear voice coil 7a, 27a upper voice coil 7b, 27b lower voice coil 17, 27 voice coil

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 マグネット(1)の上部と下部に板厚が
同じであるトッププレート(2)とボトムプレート
(3)を各々設置し、これらの外周にヨーク(4)を設
置して上部磁気ギャップ(5a)と下部磁気ギャップ
(5b)を有するギャップ(5)を形成するデュアルギ
ャップ磁気回路を設け、このギャップ(5)内に挿入配
置されるデュアルギャップ用リニアボイスコイル(7)
において、 互いに接続されており、同じ巻巾で巻き方向が逆である
上部ボイスコイル(7a)と下部ボイスコイル(7b)
からなり、 巻巾がトッププレート(2)の板厚と同じかより小さ
く、 上部磁気ギャップ(5a)内に挿入されている上部ボイ
スコイル(7a)の下部部分と下部磁気ギャップ(5
b)内に挿入されている下部ボイスコイル(7b)の上
部部分との巻巾が同じで、かつ、合計が一方のボイスコ
イルの巻巾と同じであることを特徴とするデュアルギャ
ップ用リニアボイスコイル。
1. A top plate (2) and a bottom plate (3) having the same plate thickness are installed on the upper and lower parts of a magnet (1), respectively, and a yoke (4) is installed on the outer periphery of these plates, and the upper magnet (1) is attached. A dual gap magnetic circuit for forming a gap (5) having a gap (5a) and a lower magnetic gap (5b) is provided, and a dual gap linear voice coil (7) inserted and arranged in the gap (5).
In, the upper voice coil (7a) and the lower voice coil (7b) are connected to each other and have the same winding width but opposite winding directions.
And the winding width is equal to or smaller than the plate thickness of the top plate (2), and the lower part of the upper voice coil (7a) and the lower magnetic gap (5) are inserted into the upper magnetic gap (5a).
b) A linear voice for a dual gap, which has the same winding width as the upper part of the lower voice coil (7b) inserted in b) and has the same total winding width as one voice coil. coil.
JP34731595A 1995-12-13 1995-12-13 Linear voice coil for dual gap Expired - Fee Related JP3598423B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP34731595A JP3598423B2 (en) 1995-12-13 1995-12-13 Linear voice coil for dual gap

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP34731595A JP3598423B2 (en) 1995-12-13 1995-12-13 Linear voice coil for dual gap

Publications (2)

Publication Number Publication Date
JPH09163495A true JPH09163495A (en) 1997-06-20
JP3598423B2 JP3598423B2 (en) 2004-12-08

Family

ID=18389395

Family Applications (1)

Application Number Title Priority Date Filing Date
JP34731595A Expired - Fee Related JP3598423B2 (en) 1995-12-13 1995-12-13 Linear voice coil for dual gap

Country Status (1)

Country Link
JP (1) JP3598423B2 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006148447A (en) * 2004-11-18 2006-06-08 Pioneer Electronic Corp Loudspeaker system
JP2006527933A (en) * 2003-06-18 2006-12-07 余姚温度メーター工場有限責任公司 Low inductance electromagnetic driver with non-excited magnetic circuit
JP2009089260A (en) * 2007-10-02 2009-04-23 Yamaha Corp Speaker unit and speaker instrument

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006527933A (en) * 2003-06-18 2006-12-07 余姚温度メーター工場有限責任公司 Low inductance electromagnetic driver with non-excited magnetic circuit
JP2006148447A (en) * 2004-11-18 2006-06-08 Pioneer Electronic Corp Loudspeaker system
JP2009089260A (en) * 2007-10-02 2009-04-23 Yamaha Corp Speaker unit and speaker instrument

Also Published As

Publication number Publication date
JP3598423B2 (en) 2004-12-08

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