JPS5859697A - Plane speaker - Google Patents
Plane speakerInfo
- Publication number
- JPS5859697A JPS5859697A JP15829081A JP15829081A JPS5859697A JP S5859697 A JPS5859697 A JP S5859697A JP 15829081 A JP15829081 A JP 15829081A JP 15829081 A JP15829081 A JP 15829081A JP S5859697 A JPS5859697 A JP S5859697A
- Authority
- JP
- Japan
- Prior art keywords
- diaphragm
- damper
- flat
- shaped
- speaker
- 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.)
- Pending
Links
Classifications
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04R—LOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; DEAF-AID SETS; PUBLIC ADDRESS SYSTEMS
- H04R7/00—Diaphragms for electromechanical transducers; Cones
- H04R7/26—Damping by means acting directly on free portion of diaphragm or cone
Landscapes
- Engineering & Computer Science (AREA)
- Multimedia (AREA)
- Physics & Mathematics (AREA)
- Acoustics & Sound (AREA)
- Signal Processing (AREA)
- Diaphragms For Electromechanical Transducers (AREA)
Abstract
Description
【発明の詳細な説明】
本発明は平板状の振動板をボイスコイルで直接駆動する
動電型の平板スピーカに関するものであって、その目的
とするところは、平板振動板の高域限界周波数を高くし
て、再生周波数帯域を広げるととKある、
平板振動板にボイスコイルを直接、結合し、振動板の外
周をフリーな状態にした従来の平板スピーカの高域限界
周波数は、振動板単品の一次共振周波数とはソ一致する
。その理由は、−次共振が起るとその節が円形振動板の
場合は直 、径の約2A付近のところKt53す、節の
内外の面積が+t ’x等しくなるため、−次共振周波
数以上の周波数振動は実効的な振動面積が大巾に減少し
、−次共振前の音圧レベルとの間に大きな差(10(1
1前後)が生じ、実質的に一次共振周波数以上の周波数
の音は再生していない状態と轡しい状態となるからであ
る。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an electrodynamic flat speaker in which a flat diaphragm is directly driven by a voice coil, and its purpose is to increase the high frequency limit of the flat diaphragm. The high limit frequency of a conventional flat plate speaker, in which the voice coil is directly coupled to a flat diaphragm and the outer circumference of the diaphragm is free, is the same as that of a single diaphragm. The primary resonance frequency of The reason for this is that when negative-order resonance occurs, if the node is a circular diaphragm, the area of the inside and outside of the node is equal to +t'x, so if the node is a circular diaphragm, the area of the inside and outside of the node is equal to +t' For frequency vibrations, the effective vibration area is greatly reduced, and there is a large difference (10(1)
1) occurs, and the sound with a frequency substantially higher than the primary resonance frequency is in a state where it is incorrect to say that it is not being reproduced.
本発明はこの点にかんがみ、−次共振の節が振動板の外
周により近接するようKすると共に、−次共振を含め、
高次の共振が発生した場合にこ幻を制動することができ
る構造とするととKよつて高域限界周波数を高め、再生
周波数帯域を広げることを意図する亀のであって、平板
振動板をボイスコイルで直接駆動する動電型の子機スピ
ーカにおいて、平板振動板のエッジヲ含む外周の一部又
は全部にゴムを代表とする粘弾性物質よりなるリング状
又は円弧状のダンパを接合し、2前記振動板の外周辺を
前記ダンパを介してフレームにより半固定状態に支持す
ることを特徴とする。In view of this point, the present invention is arranged such that the node of the -order resonance is closer to the outer circumference of the diaphragm, and also includes the -order resonance.
If the structure is designed to dampen the illusion when high-order resonance occurs, it is intended to raise the high limit frequency and widen the reproduction frequency band, and the flat diaphragm is used as a voice. In an electrodynamic slave speaker that is directly driven by a coil, a ring-shaped or arc-shaped damper made of a viscoelastic material such as rubber is bonded to part or all of the outer periphery including the edge of the flat diaphragm, and 2. The diaphragm is characterized in that the outer periphery of the diaphragm is semi-fixedly supported by a frame via the damper.
本発明の実施例を図面によって説明する。第1図におい
て、1はトッププレート、2はマグネット、5はポール
ピース付プレートでとわらにより磁気回路を構成してい
る。4はポールピースとトッププレート1との間に形成
される磁気間隙に配置されたボイスコイルで、そのボイ
スコイルボビン5の上端は平板振動板6に!!合さねて
いる。7は平板振動板6のエツジ、8はトッププレー)
IK固定されたフレームである。Embodiments of the present invention will be described with reference to the drawings. In FIG. 1, 1 is a top plate, 2 is a magnet, and 5 is a plate with a pole piece, which constitutes a magnetic circuit using straw. 4 is a voice coil placed in the magnetic gap formed between the pole piece and the top plate 1, and the upper end of the voice coil bobbin 5 is connected to the flat diaphragm 6! ! It doesn't match. 7 is the edge of the flat diaphragm 6, 8 is the top play)
This is a fixed IK frame.
9はエツジ7に貼看又は塗着されたゴムを代表とする粘
弾性材料よりなるリング状又は円弧状のダンパで、その
内辺は振動板6の外周辺の全周又は一部に接着され、外
辺はフレーム8に固定されている。したがって平板振動
板6はダンパ9を介してフレーム8に半固定状態で支持
される。第1図0)&Cおいてdは円弧状のダンパ9を
使用した場合に、ダンパのない部分を示している。第2
図は形状および取付力法の異なる各樵ダンパの実施例を
示している。(イ)は断面方形のリング状又は円弧状の
ダンパ9で平板振動板6を下から支持した場合、IP)
は断面長方形のリング状又は円弧状のダンパ9を平板振
動板6の周辺の端面に接合した場合、f→は断面長方形
のリング状又は円弧状のダンパ9で平板振動J#L6の
周辺の表面を支持した場合、に)および(ホ)は断面L
!i!のリング状又は円弧状のダンパ9で平板振動板6
の外周辺を支持した場合である。Reference numeral 9 denotes a ring-shaped or arc-shaped damper made of a viscoelastic material, typically rubber, which is pasted or painted on the edge 7, and whose inner side is glued to the entire or part of the outer periphery of the diaphragm 6. , the outer edge is fixed to the frame 8. Therefore, the flat diaphragm 6 is semi-fixedly supported by the frame 8 via the damper 9. In FIG. 10)&C, d indicates a portion without a damper when an arc-shaped damper 9 is used. Second
The figures show examples of lumber dampers with different shapes and mounting forces. (A) is a case where the flat plate diaphragm 6 is supported from below by a ring-shaped or arc-shaped damper 9 with a square cross section, IP)
When a ring-shaped or arc-shaped damper 9 with a rectangular cross section is joined to the peripheral end face of the flat plate diaphragm 6, f → is the ring-shaped or circular arc-shaped damper 9 with a rectangular cross section and the peripheral surface of the flat plate vibration J#L6. ) and (e) are the cross-sections L
! i! The flat plate diaphragm 6 is a ring-shaped or arc-shaped damper 9.
This is the case when the outer periphery of
以上述べたように1本発明の平板振動板はその外周辺が
半固定状態に支持されているので、−次共振が発生した
ときは、平板釉動板の外周をフリー和した従来の平板ス
ピーカに比べて節の直径が大となり、節の内外の面積は
内面積の方が外面積よりも大となり、−次共振後の音圧
レベルの低下が小さくなる。また、平板振動板の外周が
制動されているため、共振によって生ずる特性のディッ
プが改善さね、特性的に、低域から一次共振後の周波数
まで平滑に再生することが可能となる。実験の結果、第
6図に示すように、外周辺をフリーにした従来の平板振
動板を用いた平板スピーカに比し、−次共振一波数以上
の周波数帯域において15〜2倍の再生帯域かえられる
仁とを確認した。第5図0)は平板振動板6のエツジ7
にダンパ9を接合しだ第1図の実施例の音圧、周波数特
性であり、同図←)は平板振動板6の外周辺にダンパ9
を接合した第2図0)の実施例の音圧、周波数特性であ
る。As mentioned above, since the outer periphery of the flat diaphragm of the present invention is supported in a semi-fixed state, when -order resonance occurs, the flat plate diaphragm of the present invention can be replaced by a conventional flat plate speaker in which the outer periphery of the flat glazed diaphragm is free-circuited. The diameter of the node is larger than that of the node, and the inner and outer areas of the node are larger than the outer area, and the drop in the sound pressure level after -th order resonance is reduced. Furthermore, since the outer periphery of the flat diaphragm is damped, dips in characteristics caused by resonance are not improved, and smooth reproduction from low frequencies to frequencies after primary resonance is possible. As a result of the experiment, as shown in Figure 6, compared to a flat-plate speaker using a conventional flat-plate diaphragm with a free outer periphery, the reproduction band can be changed by 15 to 2 times in the frequency band above the -order resonance wave number. I confirmed that it was true. Figure 5 0) shows the edge 7 of the flat diaphragm 6.
The sound pressure and frequency characteristics of the embodiment shown in FIG.
This is the sound pressure and frequency characteristics of the embodiment shown in FIG. 2 (0) in which the
同図において、点線a、a’は従来の平板振動板を用い
た平板スピーカの音圧およびインピーピー−゛ンス特性
であり、fa、fbは従来および ゛本発明の平板スピ
ーカの高域限界周波数であり、Cはインピーダンス特性
の乱れを制動していることを示している。In the same figure, dotted lines a and a' are the sound pressure and impedance characteristics of a flat plate speaker using a conventional flat plate diaphragm, and fa and fb are the high frequency limit frequencies of the conventional flat plate speaker and the flat plate speaker of the present invention. , and C indicates that disturbances in the impedance characteristics are damped.
以上述べたように1本発明は振動板の外周辺に粘弾性材
料よりなるダンパを接合するというきわめて簡単な手段
によって平板スピーカの再生周波数帯域を拡大すること
ができ、簡易型平板スピーカの品質を向上するすぐれた
効果を有する。As described above, the present invention can expand the reproduction frequency band of a flat speaker by the extremely simple means of joining a damper made of a viscoelastic material to the outer periphery of a diaphragm, thereby improving the quality of a simple flat speaker. It has an excellent improving effect.
第1図二本発明の平板スピーカの実施例で、(イ)は平
面図、←)は縦断側面図
#I&2図:本発明のダンパの各種実施例で(イ)←)
(ハ)に)(ホ)はその側断面図
第5 @ : N>および←)は、本発明の平板スピー
カと従来の平板スピーカとの音圧、周波
′数特性を比較するグラフである。Figure 1 2 Examples of the flat speaker of the present invention, (A) is a plan view, ←) is a longitudinal side view #I & 2: Various embodiments of the damper of the present invention (A) ←)
(C)) (E) is a side sectional view thereof. No. 5 @: N> and ←) are graphs comparing the sound pressure and frequency characteristics of the flat plate speaker of the present invention and a conventional flat plate speaker.
Claims (1)
代表とする粘弾性物質よりなるり/グ状又は円弧状のダ
ンパを接合し、前記平板振動板の外周辺を前記ダンパを
介してフレームにより半固定状態に支持し、皺平板振動
板を磁気回路の磁気空隙にはめこんだボイスコイルで駆
〆 動するように構成したことを特徴とする平板スピーカ。[Scope of Claims] A round or arc-shaped damper made of a viscoelastic material such as rubber is bonded to part or all of the outer periphery including the edges of the flat diaphragm, and the outer periphery of the flat diaphragm is A flat plate speaker characterized in that the wrinkled flat plate diaphragm is semi-fixedly supported by a frame via the damper, and is driven by a voice coil fitted into a magnetic gap of a magnetic circuit.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP15829081A JPS5859697A (en) | 1981-10-05 | 1981-10-05 | Plane speaker |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP15829081A JPS5859697A (en) | 1981-10-05 | 1981-10-05 | Plane speaker |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS5859697A true JPS5859697A (en) | 1983-04-08 |
Family
ID=15668363
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP15829081A Pending JPS5859697A (en) | 1981-10-05 | 1981-10-05 | Plane speaker |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5859697A (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5168525A (en) * | 1989-08-16 | 1992-12-01 | Georg Neumann Gmbh | Boundary-layer microphone |
JP2007519352A (en) * | 2004-01-22 | 2007-07-12 | オイ ノース ウェーブ リミテッド | Loudspeaker |
WO2013021455A1 (en) * | 2011-08-09 | 2013-02-14 | 三菱電機株式会社 | Electrodynamic sound-emitting body |
JP2013038761A (en) * | 2011-12-15 | 2013-02-21 | Mitsubishi Electric Corp | Electrodynamic sound emitting body |
-
1981
- 1981-10-05 JP JP15829081A patent/JPS5859697A/en active Pending
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5168525A (en) * | 1989-08-16 | 1992-12-01 | Georg Neumann Gmbh | Boundary-layer microphone |
JP2007519352A (en) * | 2004-01-22 | 2007-07-12 | オイ ノース ウェーブ リミテッド | Loudspeaker |
WO2013021455A1 (en) * | 2011-08-09 | 2013-02-14 | 三菱電機株式会社 | Electrodynamic sound-emitting body |
JP2013038761A (en) * | 2011-12-15 | 2013-02-21 | Mitsubishi Electric Corp | Electrodynamic sound emitting body |
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