JP2014003356A - Voice coil, magnetic circuit, speaker, sound playback system and its application device - Google Patents

Voice coil, magnetic circuit, speaker, sound playback system and its application device Download PDF

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JP2014003356A
JP2014003356A JP2012135616A JP2012135616A JP2014003356A JP 2014003356 A JP2014003356 A JP 2014003356A JP 2012135616 A JP2012135616 A JP 2012135616A JP 2012135616 A JP2012135616 A JP 2012135616A JP 2014003356 A JP2014003356 A JP 2014003356A
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voice coil
magnetic
feature
permanent magnet
voice
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Junichi Kakumoto
純一 角元
Tamaki Ishizaki
環 石崎
ze-jun Pan
ゼ ジュン パン
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Abstract

PROBLEM TO BE SOLVED: To provide a structure of a planar speaker with high efficiency, high performance, wide design flexibility, and high practical utility.SOLUTION: A plurality of voice coils in square shapes are arranged in a lattice state. Adjacent sides of the voice coil are to be overlapped. Magnetic poles in square shapes are disposed within the voice coils. A permanent magnet is disposed to each of the magnetic poles so that the adjacent magnetic poles have reversed polarity. Current polarity of the adjacent voice coils are set to reversed polarity to each other and driving force is generated in the same direction for all of the voice coils. The structure can respond to the various sizes and performance requirements by increasing the number of voice coils and magnetic circuits, as required, in a surface direction, or in a plurality of layers.

Description

請求項を含む全文を通じ、{}内の内容は{}外の内容に優先して意味を持つものとする。
請求項で定義した用語は明細書でも同様とする。
Throughout the entire sentence including the claims, the content in {} has priority over the content outside {}.
The terms defined in the claims are the same in the specification.

本案発明は{理想的な平面スピーカー、そのボイスコイル、その磁気回路}に関する。 The present invention relates to {ideal flat speaker, its voice coil, its magnetic circuit}.

高効率の平面スピーカーで重要なのは{駆動力の確保}と{振動板の剛性の確保}である。
平面という条件下での駆動力の確保は容易ではない。また、駆動力が確保できたとしても、高性能という条件下で、広い平面の軽くて高い剛性の振動板は{素材の選択や形状設計}の点で難しい課題が多い。
平面スピーカーの磁気回路の設計は、強い駆動力を必要とする場合、高い磁束密度が必要なことから、永久磁石の性能もさることながら、磁路の材料の厚みを必要とし、厚みと性能は常にトレードオフの関係にある。
What is important in a high-efficiency flat speaker is {ensuring driving force} and {securing diaphragm rigidity}.
It is not easy to secure driving force under the condition of a flat surface. Moreover, even if the driving force can be ensured, under the condition of high performance, a light and high rigidity diaphragm with a wide plane has many difficult problems in terms of {material selection and shape design}.
The design of the magnetic circuit of a flat speaker requires a high magnetic flux density when a strong driving force is required. Therefore, it requires the thickness of the magnetic path material as well as the performance of the permanent magnet. There is always a trade-off relationship.

本案発明は、駆動力が平面上に分布するスピーカーの構造に関する。電磁力を利用したスピーカーは{磁気回路とボイスコイルとそれらを支える構造部品}から構成される。スピーカーの性能は与えられたコスト制限の範囲内で、用いる資源を最大限有効利用するよう設計される。高性能化を図る際、一つの要因だけに着目しても、他の要因による制約を考慮する必要があって、全体性能を一気に上げる特効的な解決策がなかった。本案発明は、{ボイスコイルの構造}と{磁気回路の構造}双方の新たな手法を組み合わせることによって、電気音響変換器としてのスピーカーの{外形寸法設計自由度、変換効率}を飛躍的に向上させるものである。 The present invention relates to a speaker structure in which driving force is distributed on a plane. A speaker using electromagnetic force is composed of {a magnetic circuit, a voice coil, and a structural part that supports them}. Speaker performance is designed to make the best use of the resources used within the given cost limits. When trying to improve performance, even if only one factor was focused on, it was necessary to consider the constraints due to other factors, and there was no effective solution to increase the overall performance at once. The present invention dramatically improves the {external dimension design freedom, conversion efficiency} of the speaker as an electroacoustic transducer by combining both the {voice coil structure} and {magnetic circuit structure}. It is something to be made.

{薄型化、高効率化}の要望は、次の第1と第2と第3の具体的な技術的課題として表現することができる。
第1の課題は、高性能の面駆動。
{平面状に均一な駆動力が分布した面駆動であること}と{高い線形性の駆動範囲を持つこと}とを両立させる。
The demand for {thinning and high efficiency} can be expressed as the following first, second, and third specific technical issues.
The first problem is high-performance surface drive.
Both {the surface drive in which a uniform driving force is distributed in a planar shape} and {having a highly linear driving range} are made compatible.

第2の課題は、高効率の面駆動。
{全周波数範囲で強い駆動力を持つこと}と{ボイスコイルのインダクタンス成分を増大させないこと}を両立させる。
The second problem is highly efficient surface driving.
{Having strong driving force in the entire frequency range} and {not increasing the inductance component of the voice coil}.

第3の課題は、平面状の振動板の曲げ強度。
音響放射板の、{強い駆動力に耐える曲げ強度を持つこと}と{高い周波数領域での変換効率を落とさないために軽量であること}を両立させる。
The third problem is the bending strength of the planar diaphragm.
The acoustic radiation plate has both {having a bending strength that can withstand a strong driving force} and {being lightweight so as not to reduce the conversion efficiency in a high frequency region}.

以上の、第1と第2と第3の課題は常にトレードオフの関係にある複数の要因を包含して解決しなければならない。そのためには、トレードオフ条件の限界範囲を広げるべく、基本的課題が解決される必要がある。 The above first, second, and third problems must always be solved by including a plurality of factors that are in a trade-off relationship. To that end, the basic problem needs to be solved in order to expand the limit range of the trade-off conditions.

第1の課題に対し、
多数の四角形筒状のボイスコイルを格子状に配置した組みボイスコイルを使う。
隣りあうボイスコイルに流れる電流極性が互いに逆となるよう、ボイスコイルの{巻方向と配線}を構成する。各々のボイスコイルには、磁極を設け、相隣りあう磁極が逆極性となるよう、磁気回路を構成する。
For the first issue,
A combined voice coil is used in which a large number of rectangular cylindrical voice coils are arranged in a grid.
The {coil direction and wiring} of the voice coil are configured so that the polarities of the currents flowing in adjacent voice coils are opposite to each other. Each voice coil is provided with a magnetic pole, and a magnetic circuit is configured so that adjacent magnetic poles have opposite polarities.

第2の課題に対し、
小さい磁石を分布させることで、一個一個の駆動力は小さいものの、一個一個の磁気回路の磁気ギャップの磁束密度を効率よく高密度にし、ヨークは一枚の薄い平面磁路を使う。隣あうボイスコイルの電流極性が逆とすることによって、ボイスコイル間の相互インダクタンス成分を相殺する。
For the second issue,
By distributing small magnets, the driving force of each one is small, but the magnetic gap density of each magnetic circuit is efficiently increased, and the yoke uses a thin planar magnetic path. Mutual inductance components between the voice coils are canceled by reversing the current polarities of adjacent voice coils.

第3の課題に対し、
多数の四角形筒状のボイスコイル格子状に、密着配列した、組みボイスコイルは、平面スピーカーの大きな弱点である振動板の曲げ強度を補強する。
For the third issue,
The assembled voice coil arranged in close contact with a large number of rectangular cylindrical voice coil lattices reinforces the bending strength of the diaphragm, which is a major weak point of a flat speaker.

以下の第1から第9の効果がある。
第1に、平面状に駆動力が分布した面駆動。
隣りあうコイルの電流極性と、隣りあう磁極が逆極性であることから、コイルに流す電流により発生する力は、すべてのコイルユニットにおいて同じ方向となる。単位面積あたりのコイルユニットの個数を増やすことで、実用上理想的なレベルにまで駆動力を平面状に分布させることができる。面積や面の形状については再生特性を犠牲にすることなく自在に設計できる。振動板の放射面積を大きくし、振動のストロークを小さくできるので、薄形に適した手法である。さらに、磁性部品が小さいことから、磁気ギャップの磁束密度を高く設計しても、局部的に磁束が小さいことから、再生性能を犠牲にすることなく、無用な磁気回路材料が削減され、薄型構造に適している。
There are the following first to ninth effects.
First, surface driving in which driving force is distributed in a planar shape.
Since the current polarity of adjacent coils and the adjacent magnetic poles have opposite polarities, the force generated by the current flowing through the coils is in the same direction in all coil units. By increasing the number of coil units per unit area, the driving force can be distributed in a planar shape to a practically ideal level. The area and shape of the surface can be freely designed without sacrificing the reproduction characteristics. Since the radiation area of the diaphragm can be increased and the stroke of vibration can be reduced, this method is suitable for thin type. In addition, because the magnetic parts are small, even if the magnetic flux density of the magnetic gap is designed high, the magnetic flux is locally small, so that unnecessary magnetic circuit materials are reduced without sacrificing reproduction performance, and a thin structure Suitable for

第2に、全平面にわたり、{コイルの分布}と{コイルと交差するところの{強い磁束密度の領域の分布}}を高密度にすることで、強い駆動力を得ることができる。
さらに、隣りあう磁極に対応するコイルの電流極性が互いに逆であることから、{隣りあうコイルユニット間の相互インダクタンス成分}が相殺され、高い周波領域の変換効率が高い。
Secondly, a strong driving force can be obtained by increasing the density of {coil distribution} and {distribution of strong magnetic flux density region where the coil intersects} over the entire plane.
Furthermore, since the current polarities of the coils corresponding to the adjacent magnetic poles are opposite to each other, {the mutual inductance component between adjacent coil units} is canceled out, and the conversion efficiency in the high frequency region is high.

第3に、同一面積内でのコイルの長さを、組み磁気回路の周囲の長さより大幅に長くすることができることから、ボイスコイルの並列接続と直列接続を組み合わせることで要求仕様に見合ったコイル設計の自由度が高く、選択範囲が広い。 Third, since the coil length within the same area can be made significantly longer than the circumference of the assembled magnetic circuit, a coil that meets the required specifications by combining parallel connection and series connection of voice coils. The degree of freedom in design is high and the selection range is wide.

第4に、ボイスコイルのサイズを小さくし、数を増やし密度を高くすることで、同一面積内でのコイル長を大幅に長くとることができ、電気から音響へのエネルギー変換効率を大幅に改善する。 Fourth, by reducing the size of the voice coil, increasing the number and increasing the density, the coil length within the same area can be greatly increased, and the energy conversion efficiency from electricity to sound is greatly improved. To do.

第5に、ボイスコイルを面状に分散させるので、コイルの銅損による発生熱が分散し、その結果、{局部的な温度上昇による入力電力限界範囲}を広げる。 Fifth, since the voice coil is dispersed in a planar shape, heat generated by the copper loss of the coil is dispersed, and as a result, the {input power limit range due to local temperature rise} is widened.

第6に、駆動力を面分布させることができることから、基本設計を変更することなく、音響放射面の形状の選択範囲を大幅に広げる。 Sixth, since the driving force can be surface-distributed, the selection range of the shape of the acoustic radiation surface is greatly expanded without changing the basic design.

第7に、面分布状に駆動力を分散できることから、振動板の面積が広くても振動板の曲げ強度を高くする必要がない。従って、同じ音圧を得る場合、振動面積を増やし、振動振幅が小さくても済むよう設計できる。このことは低音再生能力の設計自由度を大幅に改善する。 Seventh, since the driving force can be distributed in a surface distribution, it is not necessary to increase the bending strength of the diaphragm even if the area of the diaphragm is large. Therefore, when obtaining the same sound pressure, the vibration area can be increased and the vibration amplitude can be reduced. This greatly improves the design freedom of the bass reproduction capability.

第8に、単位磁極あたりの総磁束を小さくできることから、平面磁路を薄形に設計できる。面積を広くとることで振動振幅を小さくできる効果と相まって、薄形の外観デザインの自由度を高める。 Eighth, since the total magnetic flux per unit magnetic pole can be reduced, the planar magnetic path can be designed to be thin. Combined with the effect that the vibration amplitude can be reduced by taking a large area, the degree of freedom in designing a thin external appearance is increased.

本案発明の基本構造の一実施例の説明図(a)C−C‘ 断面(b)A−A‘ 断面(c)B−B‘ 断面Explanatory drawing of one Example of basic structure of this invention (a) C-C 'cross section (b) A-A' cross section (c) B-B 'cross section 図1円内部の磁束分布と電流方向の説明図 (a)図1の円71部の拡大図 (b)図1の円72部の拡大図Fig. 1 Magnetic flux distribution and current direction inside circle (a) Enlarged view of circle 71 in Fig. 1 (b) Enlarged view of circle 72 in Fig. 1 図1の基本構造に加えて第2永久磁石を設けた本案発明の一実施例の説明図Explanatory drawing of one Example of this invention which provided the 2nd permanent magnet in addition to the basic structure of FIG. 図1の基本構造に加えて磁気回路と組ボイスコイルを2階構造とした、本案発明の一実施例の説明図。FIG. 2 is an explanatory diagram of an embodiment of the present invention in which a magnetic circuit and a set voice coil have a two-story structure in addition to the basic structure of FIG. 1.

第1に
{図1(a)に示すように、16個の四角形筒状のボイスコイルを格子状に組む。
一方、16個の四角形状の磁極を配置し、磁極間の空隙に格子状のボイスコイルを収める。全ての磁極の隣りあう磁極が互いに逆極性となるよう、永久磁石を配置し、磁極と永久磁石を平面磁路上に配置する。平面磁路の四隅を折り曲げて、外側の磁極の外側の辺との間に磁気ギャップを設ける。全てのボイスコイルの隣りあうボイスコイルは互いに逆極性となるよう、巻方向または配線を決める。即ち、全てのN磁極を取りまくボイスコイルの電流方向が左回転(右回転)のとき、全てのS磁極を取りまくボイスコイルの電流方向は右回転(左回転)である。
隣りあう磁極の極性とボイスコイルに流れる電流の極性の双方が逆であることから、全てのボイスコイルに発生する駆動力は同一方向となる。
First, as shown in FIG. 1 (a), 16 rectangular cylindrical voice coils are assembled in a lattice pattern.
On the other hand, 16 rectangular magnetic poles are arranged, and a lattice-like voice coil is accommodated in a gap between the magnetic poles. Permanent magnets are arranged such that all adjacent magnetic poles have opposite polarities, and the magnetic poles and permanent magnets are arranged on a planar magnetic path. The four corners of the planar magnetic path are bent to provide a magnetic gap between the outer sides of the outer magnetic poles. The winding direction or wiring is determined so that the voice coils adjacent to all the voice coils have opposite polarities. That is, when the current direction of the voice coil surrounding all the N magnetic poles is counterclockwise (right rotation), the current direction of the voice coil surrounding all the S magnetic poles is right rotation (left rotation).
Since both the polarity of the adjacent magnetic poles and the polarity of the current flowing in the voice coil are opposite, the driving forces generated in all the voice coils are in the same direction.

図1は16個の{ボイスコイルと磁極と永久磁石}からなるが、一般的には、用途や性能によって任意の数で構成する。 FIG. 1 is composed of 16 {voice coils, magnetic poles and permanent magnets}, but in general, it is configured with an arbitrary number depending on the application and performance.

第2に、図1の磁極の上に永久磁石を設け、磁気ギャップの磁束密度を上げ、さらなる駆動力を得る。 Second, a permanent magnet is provided on the magnetic pole of FIG. 1 to increase the magnetic flux density of the magnetic gap and obtain further driving force.

第3に、図1の磁極の上に図1と同様の永久磁石と磁極とボイスコイルを設け、さらなる駆動力を得る。 Third, a permanent magnet, a magnetic pole, and a voice coil similar to those in FIG. 1 are provided on the magnetic pole in FIG. 1 to obtain further driving force.

スピーカーの構造の一部である{エッジ、ダンパー、ボビン}については、一般のスピーカーと同様であるので、説明を省略する。 Since {edge, damper, bobbin} which is a part of the structure of the speaker is the same as that of a general speaker, description thereof is omitted.

以下、図面を用いた詳細説明。
図1は本案発明の基本構造を説明する一実施例である。
X1からX4は、図面の説明上の横軸の位置、Y1からY4は図面の説明上の縦軸の位置を示す。例えば、211の磁極の中心座標は{X1、Y1}、
242の磁極の中心座標は{X4、Y2}である。
図1は、磁極が、{縦4行、横4列}の
{16個のボイスコイル、16個の磁極、16個の永久磁石、1個の平面ヨーク、1個の振動板}からなる平面スピーカーの構造である。
Hereinafter, detailed description using drawings.
FIG. 1 shows an embodiment for explaining the basic structure of the present invention.
X1 to X4 indicate the position of the horizontal axis in the description of the drawing, and Y1 to Y4 indicate the position of the vertical axis in the description of the drawing. For example, the center coordinates of 211 magnetic poles are {X1, Y1},
The center coordinates of the magnetic pole 242 are {X4, Y2}.
FIG. 1 shows a plane in which magnetic poles are {16 voice coils, 16 magnetic poles, 16 permanent magnets, 1 plane yoke, 1 diaphragm} of {vertical 4 rows, horizontal 4 columns}. The structure of the speaker.

図1(a)は図1(b)のC−C‘断面を示す。
図1(b)は図1(a)のA−A‘断面を示す。
図1(c)は図1(a)のB−B‘断面を示す。
FIG. 1A shows a CC ′ cross section of FIG.
FIG.1 (b) shows the AA 'cross section of Fig.1 (a).
FIG.1 (c) shows the BB 'cross section of Fig.1 (a).

111、121、141、142は、それぞれ座標{x1,y1}、{x2、Y1}、{X4、Y1}、{X4、Y2}に位置するボイスコイル、
各コイルユニットの4辺に示す{太い線と太い矢印}は、その磁気ギャップのボイスコイルの電流極性を示す。
211、221、231、241、242、243は、それぞれ
座標{x1,y1}、{x2、Y1}、{X3、Y1}、{X4、Y1}、{X4、Y2}、{X4、Y3}に位置する磁極、
311、321、341、342、343は、それぞれ
座標{x1,y1}、{x2、Y1}、{X4、Y1}、{X4、Y2}、{X4、Y3}に位置する永久磁石、
4は平面磁路、
511、512、513、515はボイスコイルのボビンのA−A‘断面、
521、522、523、525はボイスコイルのボビンのB−B‘断面、
6は振動板である。
71と72の円で囲む部分は{後述の図2の拡大図での詳細説明}の部分である。
白丸はボイスコイルの電流極性が{手前から向こう}を向いていることを示す。黒丸はボイスコイルの電流極性が{向こうから手前}を向いていることを示す。
111, 121, 141, 142 are voice coils located at coordinates {x1, y1}, {x2, Y1}, {X4, Y1}, {X4, Y2}, respectively.
The {thick line and thick arrow} on the four sides of each coil unit indicate the current polarity of the voice coil in the magnetic gap.
211, 221, 231, 241, 242, and 243 are coordinates {x1, y1}, {x2, Y1}, {X3, Y1}, {X4, Y1}, {X4, Y2}, {X4, Y3}, respectively. Magnetic poles located at the
311, 321, 341, 342, 343 are permanent magnets located at coordinates {x1, y1}, {x2, Y1}, {X4, Y1}, {X4, Y2}, {X4, Y3},
4 is a plane magnetic path,
511, 512, 513, 515 are AA ′ cross-sections of the bobbin of the voice coil,
521, 522, 523, 525 are BB ′ cross-sections of the bobbin of the voice coil,
6 is a diaphragm.
A portion surrounded by circles 71 and 72 is a portion {detailed explanation in an enlarged view of FIG. 2 described later}.
A white circle indicates that the current polarity of the voice coil is facing from the front. A black circle indicates that the current polarity of the voice coil is facing from the front to the front.

ボイスコイルは、
横座標{X1、X2、X3、X4}と縦座標{Y1、Y2、Y3、Y4}の交差点を中心とする位置に設ける。隣りあうボイスコイルの電流極性が互いに逆方向となるよう{巻方向と配線}によって電流極性を決定する。
隣りあう磁極は互いに逆極性となるよう配置する。N極の磁極の周りの全ての磁極はS極で、S極の磁極の周りの全ての磁極はN]極である。
Voice coil
It is provided at a position centering on the intersection of the abscissa {X1, X2, X3, X4} and the ordinate {Y1, Y2, Y3, Y4}. The current polarity is determined by {winding direction and wiring} so that the current polarities of adjacent voice coils are opposite to each other.
Adjacent magnetic poles are arranged to have opposite polarities. All poles around the N pole are S poles and all poles around the S pole are N] poles.

ボイスコイル221は上面からみて右巻極性であって、ボイスコイルが囲む磁極はN極であり、矢印方向に電流を流した場合振動板を押し出す方向に駆動力が発生する。ボイスコイル211は上面からみて左巻極性であって、ボイスコイルが囲む磁極はS極であり、矢印方向に電流を流した場合振動板を押し出す方向に駆動力が発生する。同様に全てのボイスコイルに同一電流をその方向に流した場合、全てのボイスコイルは振動板を押し出す方向に駆動力を発生する。 The voice coil 221 has a right-handed polarity when viewed from above, and the magnetic pole surrounded by the voice coil is an N pole. When a current is passed in the direction of the arrow, a driving force is generated in the direction of pushing out the diaphragm. The voice coil 211 has a left-handed polarity when viewed from above, and the magnetic pole surrounded by the voice coil is an S pole. When a current is passed in the direction of the arrow, a driving force is generated in the direction of pushing out the diaphragm. Similarly, when the same current is supplied to all voice coils in that direction, all voice coils generate a driving force in the direction of pushing out the diaphragm.

隣りあう磁極間の磁気ギャップには均一な磁界が発生し、ボイスコイルに流す電流はボイスコイル全体に均一な駆動力を生む。 A uniform magnetic field is generated in the magnetic gap between adjacent magnetic poles, and the current flowing through the voice coil produces a uniform driving force throughout the voice coil.

図2は図1の円で囲った部分{71と72}の磁極間の磁束分布の説明図である。
図2(a)は図1の71の部分、図2(b)は図1の72の部分を示す。
図2の{図1と同番号}は同機能である。
232は図1の{X3、Y2}座標のN磁極であり、
その四方を{222,231、242、233}のS極が取り囲んでいる。
{241、242,243}はそれぞれ
座標{X4、Y1}{X4、Y2}{X4、Y3}の上にあって、{N、S、N}の磁極である。
{341、342、343}は座標{X4、Y1}{X4、Y2}{X4、Y3}の永久磁石である。
{細い線と細い矢印}の組みは、磁路内の{磁束と磁束の方向}を示す。
上面から見た{NからSへ向かう磁束}は4辺間では平行に近いが、4個の磁極のコーナーが集まる空間ではギャップからはみ出るように膨らむ。ボイスコイルは、この部分では四半円であり、磁束とほぼ直交するのでこの四半円の部分も、効率を大きく落とすことなく、駆動力を生む。
FIG. 2 is an explanatory diagram of the magnetic flux distribution between the magnetic poles of the portions {71 and 72} surrounded by a circle in FIG.
2A shows a portion 71 in FIG. 1, and FIG. 2B shows a portion 72 in FIG.
2 has the same function.
Reference numeral 232 denotes the N magnetic pole of the {X3, Y2} coordinate in FIG.
The S poles {222, 231, 242, 233} surround the four sides.
{241, 242, 243} are magnetic poles of {N, S, N} on coordinates {X4, Y1} {X4, Y2} {X4, Y3}, respectively.
{341, 342, 343} are permanent magnets having coordinates {X4, Y1} {X4, Y2} {X4, Y3}.
A set of {thin line and thin arrow} indicates {magnetic flux and direction of magnetic flux} in the magnetic path.
The {magnetic flux from N to S} viewed from above is nearly parallel between the four sides, but swells out of the gap in the space where the corners of the four magnetic poles gather. The voice coil is a quarter circle in this portion and is almost orthogonal to the magnetic flux, so that this quarter circle portion also generates a driving force without greatly reducing the efficiency.

{241と242の磁極間の磁束}は{341と342の永久磁石}と4の平面磁路を磁路とする磁気ループによって生じる。本案発明の磁気回路は、一般のスピーカーの磁気回路のように、{大きな一個の磁石からの磁束}を導く磁路ではなく、小さい磁石が分散されて、小さい磁極に導く磁路であって、磁路中の磁束は小さい。磁路も分散されていることから、断面積の大きい磁路を必要としない。従って、薄い板状の平面磁路で機能させることができ、磁気回路材料の無駄が少なく、薄形のスピーカーに適している。 The {magnetic flux between the magnetic poles of 241 and 242} is generated by a magnetic loop having a {341 and 342 permanent magnet} and a plane magnetic path of 4 as a magnetic path. The magnetic circuit of the present invention is not a magnetic path for guiding {magnetic flux from one large magnet} like a general speaker magnetic circuit, but a magnetic path in which small magnets are dispersed and led to small magnetic poles, The magnetic flux in the magnetic path is small. Since the magnetic path is also dispersed, a magnetic path having a large cross-sectional area is not required. Therefore, it can function with a thin plate-like planar magnetic path, and there is little waste of magnetic circuit material, which is suitable for a thin speaker.

図3は本案発明の一実施例を示す。図1の基本構造に加え、磁極間の磁気ギャップの磁束密度をさらに高めるための手法である。図1、図2と同番号は同機能を示す。3011,3021、3031、3041はそれぞれ第2永久磁石である。
第1永久磁石{311、321、331、341}と
第2永久磁石{3011、3021、3031、3041}は、それぞれ、
磁極{211、221、231、241}側で同極性である。第2永久磁石を設けることで、磁気ギャップの磁束密度を約2倍に上げることができる。
{薄形化、高性能化}に効果的な手法である。
FIG. 3 shows an embodiment of the present invention. This is a technique for further increasing the magnetic flux density of the magnetic gap between the magnetic poles in addition to the basic structure of FIG. 1 and 2 indicate the same function. Reference numerals 3011, 3021, 3031, and 3041 denote second permanent magnets.
The first permanent magnet {311, 321, 331, 341} and the second permanent magnet {3011, 3021, 3031, 3041}
It has the same polarity on the magnetic pole {211, 221, 231, 241} side. By providing the second permanent magnet, the magnetic flux density of the magnetic gap can be increased approximately twice.
This is an effective technique for {thinning and high performance}.

図4は本案発明の一実施例を示す。図1の基本構造に加え、さらに1段の{磁気ギャップとボイスコイル}を設け、駆動力を増強する場合の説明図である。
図4の図1、図2、図3と同番号は同機能である。
2011、2021、2031、2041は第2磁極、
図1に説明の第1組ボイスコイルに加え、第2組ボイスコイルを2階建て構造に設けることから駆動力が大きくなる。図3では,第2永久磁石の第1磁極と反対側の磁極から出る磁束を駆動力に利用していないが、図4ではその磁束を第2磁極の磁気ギャップに集中させ、磁束の利用効率を上げる。図4の方法は図3の方法に比べ駆動力を約1.5倍とすることができる。
FIG. 4 shows an embodiment of the present invention. FIG. 2 is an explanatory diagram in the case of further increasing the driving force by providing one stage {magnetic gap and voice coil} in addition to the basic structure of FIG. 1.
The same numbers as those in FIGS. 1, 2, and 3 in FIG. 4 indicate the same functions.
2011, 2021, 2031, and 2041 are second magnetic poles,
Since the second voice coil is provided in the two-story structure in addition to the first voice coil described in FIG. 1, the driving force is increased. In FIG. 3, the magnetic flux from the magnetic pole opposite to the first magnetic pole of the second permanent magnet is not used as the driving force, but in FIG. 4, the magnetic flux is concentrated in the magnetic gap of the second magnetic pole, and the use efficiency of the magnetic flux Raise. The method of FIG. 4 can increase the driving force by about 1.5 times compared to the method of FIG.

さらに図3と同様、第2磁極の上面に第3の永久磁石を設けることで図3に比べ駆動力を約2倍とすることができる。
さらに、ボイスコイルと磁気回路の階層を増やすことで駆動力を上げることができる。
Further, similarly to FIG. 3, by providing a third permanent magnet on the upper surface of the second magnetic pole, the driving force can be approximately doubled compared to FIG.
Furthermore, driving force can be increased by increasing the hierarchy of voice coils and magnetic circuits.

請求項1はボイスコイルの構造に関する。四角形状のボイスコイルを組み合わせることで、有効な駆動力を得るボイスコイルの密度を上げる手法に関する。
請求項2は上記ボイスコイルと組み合わせる磁気回路に関する。各ボイスコイルに対応して磁極と永久磁石と共通の平面磁路を設けることで、面駆動系が完成する。
請求項3は磁気ギャップの磁束密度を上げ、駆動力をさらに上げる方法に関する。
請求項4はボイスコイルと磁気回路を2階層にすることで、駆動力をさらに上げる方法に関する。
請求項5は2階層目の磁気ギャップの磁束密度を上げ、ボイスコイルと磁気回路の駆動力を、さらに上げる方法に関する。
請求項6は任意の階層のボイスコイルと磁気回路により、駆動力を上げる方法に関する。
請求項7は請求項1から請求項6に定義の部品としてのスピーカーを音響再生装置、あるいはその応用装置への応用に関する。
Claim 1 relates to the structure of the voice coil. The present invention relates to a method for increasing the density of a voice coil that obtains an effective driving force by combining rectangular voice coils.
Claim 2 relates to a magnetic circuit combined with the voice coil. A plane driving system is completed by providing a plane magnetic path common to the magnetic pole and the permanent magnet corresponding to each voice coil.
The third aspect relates to a method for increasing the magnetic flux density of the magnetic gap and further increasing the driving force.
A fourth aspect of the present invention relates to a method for further increasing the driving force by making the voice coil and the magnetic circuit into two layers.
The fifth aspect relates to a method of increasing the magnetic flux density of the magnetic gap in the second layer and further increasing the driving force of the voice coil and the magnetic circuit.
A sixth aspect of the present invention relates to a method for increasing a driving force by using a voice coil and a magnetic circuit in an arbitrary hierarchy.
A seventh aspect of the present invention relates to an application of a speaker as a component defined in the first to sixth aspects to a sound reproducing device or an application device thereof.

X1、X2、X3、X4 図面の横軸の位置。
Y1、Y2、Y3、Y4 図面の縦軸の位置。
111,121、131、132、133、141、142 ボイスコイル。
太い線と太い矢印 ボイスコイルとその電流極性。
細い線と細い矢印 磁束とその方向。
211、221、231、241、222,232、233、242、243
第1磁極。
2011、2021、2031、2041 第2磁極。
311、321、341、342、343 第1永久磁石。
3011、3021、3031、3041 第2永久磁石。
4 平面磁路。
511、512、513、515、521、522、523、525、ボビン。
6 振動板。
71、72 拡大図のエリア。












X1, X2, X3, X4 Position on the horizontal axis of the drawing.
Y1, Y2, Y3, Y4 Position of the vertical axis in the drawing.
111, 121, 131, 132, 133, 141, 142 Voice coils.
Thick line and thick arrow Voice coil and its current polarity.
Thin line and thin arrow Magnetic flux and its direction.
211, 221, 231, 241, 222, 232, 233, 242, 243
First magnetic pole.
2011, 2021, 2031, 2041 The second magnetic pole.
311, 321, 341, 342, 343 First permanent magnet.
3011, 3021, 3031, 3041 Second permanent magnet.
4 Planar magnetic path.
511, 512, 513, 515, 521, 522, 523, 525, bobbin.
6 Diaphragm.
71, 72 Enlarged area.












Claims (7)

四角形筒状のボイスコイルをボイスコイルとし、
複数のボイスコイルの四角形の辺どうしが隣り合わせに重なるようボイスコイルを振動板上に格子状に配置することを第1の特徴とし、
ボイスコイルが振動板に配置されている状態で、ボイスコイルの振動板側から見た状態を上面とし、
全てのボイスコイルに同一電流を流した場合、
上面から見て、電流の方向が反時計回りを左回りとし、その逆方向を右回りとし、
上面から見て、電流の方向が左回りであるグループを{左巻きボイスコイル}とし、
上面から見て、電流の方向が右回りであるグループを{右巻きボイスコイル}とし、
ボイスコイルを振動板に配置した状態で、全ての左巻ボイスコイルの隣のボイスコイルが全て右巻きボイスコイルであって、全ての右巻きボイスコイルの隣のボイスコイルは全て左巻ボイスコイルであることを第2の特徴とし、
隣りあうボイスコイルの一辺どうしが密着されていることを第3の特徴とし、
第2の特徴の結果ではあるが、{密着された双方のボイスコイルに流れる電流}の方向が同じ向きであることを第4の特徴とし、
全てのボイスコイルが組み合わさったものを組みボイスコイルとし、
上記第1と第2と第3と第4の特徴を有する組みボイスコイルまたは振動板に装着された組みボイスコイル。
A rectangular cylindrical voice coil is used as a voice coil.
The first feature is that the voice coils are arranged in a lattice pattern on the diaphragm so that the rectangular sides of the plurality of voice coils overlap each other.
With the voice coil placed on the diaphragm, the state seen from the diaphragm side of the voice coil is the top surface,
When the same current is applied to all voice coils,
When viewed from the top, the current direction is counterclockwise counterclockwise and the opposite direction clockwise.
A group in which the current direction is counterclockwise when viewed from above is {left-handed voice coil},
A group in which the direction of current is clockwise when viewed from above is {right-handed voice coil},
With the voice coil placed on the diaphragm, all voice coils next to all left-handed voice coils are right-handed voice coils, and all voice coils next to all right-handed voice coils are left-handed voice coils. The second feature is that
The third feature is that the sides of adjacent voice coils are in close contact with each other.
As a result of the second feature, the fourth feature is that the directions of {the currents flowing through both of the closely attached voice coils} are the same,
A combination of all voice coils is used as a voice coil.
A combined voice coil having the above first, second, third and fourth characteristics or a combined voice coil mounted on a diaphragm.
請求項1に定義の一個のボイスコイルの内側の四角形筒状の空間に収める四角形状の磁性材料を磁極とし、
組みボイスコイルを構成するそれぞれのボイスコイルに磁極が収まるよう磁極が配列されていることを第5の特徴とし、
隣りあうボイスコイルの一辺どうしが密着した辺を密着辺とし、
全ての密着辺が双方の磁極間の磁気ギャップに収まる構造であることを第6の特徴とし、
隣りあう磁極が逆極性となるようそれぞれの磁極に{柱状または平板状}の永久磁石を配置することを第7の特徴とし、
上記、永久磁石を永久磁石とし、
{永久磁石と磁極を組み合わせたもの}を{各ボイスコイルに対応させ配列し配置するための板状の磁性材料}を平面磁路とし、
永久磁石が平面磁路に密着していることを第8の特徴とし、
それぞれの磁極が、それぞれの永久磁石と平面磁路を介して磁気的に結合された構造体を{組み磁気回路}とし、
隣りあう磁極間の磁気ギャップに、請求項1の組みボイスコイルの全ての辺が挿入され、{磁化された磁極による磁極間の磁束の方向}と{ボイスコイルに流れる電流の方向}が垂直に交差するよう、{組み磁気回路}の磁極が配列されていることを第9の特徴とし、
上記第5と第6と第7と第8と第9の特徴を有するスピーカー。
A quadrangular magnetic material that fits in a rectangular cylindrical space inside one voice coil as defined in claim 1 is used as a magnetic pole.
The fifth feature is that the magnetic poles are arranged so that the magnetic poles are accommodated in each voice coil constituting the assembled voice coil,
The side where adjacent sides of the voice coil are in close contact is defined as the close contact side.
The sixth feature is that all the contact edges fit in the magnetic gap between the magnetic poles.
A seventh feature is that {columnar or flat plate} permanent magnets are arranged on each magnetic pole so that adjacent magnetic poles have opposite polarities,
The permanent magnet is a permanent magnet,
{The combination of permanent magnets and magnetic poles} is {plate-like magnetic material for arranging and arranging corresponding to each voice coil} as a planar magnetic path,
The eighth feature is that the permanent magnet is in close contact with the planar magnetic path,
A structure in which each magnetic pole is magnetically coupled to each permanent magnet through a planar magnetic path is referred to as a {assembled magnetic circuit}.
All sides of the assembled voice coil of claim 1 are inserted into the magnetic gap between adjacent magnetic poles, and {the direction of magnetic flux between the magnetic poles by the magnetized magnetic pole} and {the direction of current flowing through the voice coil} are perpendicular to each other The ninth feature is that the magnetic poles of {assembled magnetic circuit} are arranged so as to intersect,
A speaker having the fifth, sixth, seventh, eighth and ninth characteristics.
請求項2に定義する永久磁石を第1永久磁石とし、
{請求項2に定義する磁極の、第1永久磁石の面と反対側の面}に第2永久磁石を配置することを第10の特徴とし、
第1永久磁石と第2永久磁石の双方の極性は磁極側で同一極性であるものとし、
第10の特徴を有するスピーカー
The permanent magnet defined in claim 2 is a first permanent magnet,
The tenth feature is that the second permanent magnet is disposed on the surface of the magnetic pole defined in claim 2 on the side opposite to the surface of the first permanent magnet,
The polarity of both the first permanent magnet and the second permanent magnet shall be the same polarity on the magnetic pole side,
Speaker having tenth feature
請求項2に定義する磁極を第1磁極とし、
{請求項3に定義する第2永久磁石の、第1磁極と反対側の面}の側に第2磁極を配置したことを第11の特徴とし、
請求項1に定義する組みボイスコイルを第1組みボイスコイルとし、
第1組みボイスコイルに加えて、隣りあう第2磁極間の磁気ギャップに、{第1組ボイスコイルと同構造の第2組みボイスコイル}を配置したことを第12の特徴とし、
第1組ボイスコイルと第2組ボイスコイルを構成する同一軸上の一対のボイスコイルは同一ボビンに構成されているとし、
第1組ボイスコイルと第2組ボイスコイルを構成する全てのボイスコイルに発生する力は、同一電流により同じ方向であるよう電流極性が決定されているとし、
第11と第12の特徴を有するスピーカー。
The magnetic pole defined in claim 2 is a first magnetic pole,
The eleventh feature is that the second magnetic pole is disposed on the side of the {second surface of the second permanent magnet defined in claim 3 opposite to the first magnetic pole},
The assembled voice coil defined in claim 1 is a first assembled voice coil,
In addition to the first voice coil, a twelfth feature is that {second voice coil having the same structure as the first voice coil} is arranged in the magnetic gap between the adjacent second magnetic poles.
A pair of voice coils on the same axis constituting the first voice coil and the second voice coil are configured on the same bobbin.
It is assumed that the current polarity is determined so that the forces generated in all the voice coils constituting the first voice coil and the second voice coil are in the same direction by the same current,
A speaker having eleventh and twelfth characteristics.
請求項4の第2磁極の{第2永久磁石の反対側の面}に第3永久磁石を配置したことを第13の特徴とし、
第3永久磁石の第2磁極側の極性は第2永久磁石の極性と同じであるとし、
第13の特徴を有するスピーカー。
A thirteenth feature is that a third permanent magnet is disposed on the {opposite surface of the second permanent magnet} of the second magnetic pole of claim 4;
The polarity on the second magnetic pole side of the third permanent magnet is the same as the polarity of the second permanent magnet,
A speaker having a thirteenth feature.
請求項4と請求項5に定義するところの、{第1と第2}の{永久磁石と磁極と組みボイスコイル}からなる二つの駆動力を生む構造を2階構造とし、
2階構造を、さらに3階構造、4階構造と、任意の階層構造としたことを第14の特徴とし、
第14の特徴を有するスピーカー
As defined in claim 4 and claim 5, the structure that produces two driving forces consisting of {first and second} {permanent magnet and magnetic pole and assembled voice coil} is a second floor structure,
The 14th feature is that the second-floor structure is further changed to a third-floor structure, a fourth-floor structure, and an arbitrary hierarchical structure.
Speaker having fourteenth feature
請求項2と請求項3と請求項4と請求項5と請求項6に定義するスピーカーを有することを第15の特徴とする、{音響再生装置}と、その音響再生装置を有する{車、テレビジョンセット、ラジオセット、通話装置、モバイルプレーヤ}



A fifteenth feature having a speaker as defined in claim 2, claim 3, claim 4, claim 5 and claim 6, {sound reproduction device}, and {sound car comprising the sound reproduction device} Television set, radio set, telephone equipment, mobile player}



JP2012135616A 2012-06-15 2012-06-15 Voice coil, magnetic circuit, speaker, sound playback system and its application device Pending JP2014003356A (en)

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JP2003179994A (en) * 2001-10-04 2003-06-27 Fps:Kk Diaphragm for planar acoustic transducer, and planar acoustic transducer
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CN107483751A (en) * 2017-07-05 2017-12-15 广东欧珀移动通信有限公司 Terminal device and its power energy allocation method, computer-readable recording medium
CN107483751B (en) * 2017-07-05 2020-10-02 Oppo广东移动通信有限公司 Terminal device, electric quantity distribution method thereof and computer-readable storage medium

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