JPH0129920Y2 - - Google Patents

Info

Publication number
JPH0129920Y2
JPH0129920Y2 JP15665480U JP15665480U JPH0129920Y2 JP H0129920 Y2 JPH0129920 Y2 JP H0129920Y2 JP 15665480 U JP15665480 U JP 15665480U JP 15665480 U JP15665480 U JP 15665480U JP H0129920 Y2 JPH0129920 Y2 JP H0129920Y2
Authority
JP
Japan
Prior art keywords
diaphragm
rectangular flat
coil bobbin
speaker
flat plate
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
JP15665480U
Other languages
Japanese (ja)
Other versions
JPS5780995U (en
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 filed Critical
Priority to JP15665480U priority Critical patent/JPH0129920Y2/ja
Publication of JPS5780995U publication Critical patent/JPS5780995U/ja
Application granted granted Critical
Publication of JPH0129920Y2 publication Critical patent/JPH0129920Y2/ja
Expired legal-status Critical Current

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  • Audible-Bandwidth Dynamoelectric Transducers Other Than Pickups (AREA)
  • Diaphragms For Electromechanical Transducers (AREA)

Description

【考案の詳細な説明】 本考案は矩形平板振動板を用いる動電型スピー
カに関し、高域の再生帯域を拡大できる高性能な
動電型スピーカを提供するものである。
[Detailed Description of the Invention] The present invention relates to an electrodynamic speaker using a rectangular flat diaphragm, and provides a high-performance electrodynamic speaker that can expand the high frequency reproduction band.

第1図A,Bは矩形平板振動板を用いた従来の
動電型スピーカを示している。第1図A,Bにお
いて、1はセンターポール2が一体に形成された
ヨーク、3はヨーク1上に固定された環状のマグ
ネツト、4はマグネツト3上に固定された環状の
プレートであり、このプレート4の内周面とセン
ターポール2の外周面との間に環状の磁気ギヤツ
プが形成されている。5はフレームであり、磁気
回路を構成する上記ヨーク1は上記フレーム5の
内部底面に固定されている。6は矩形平板振動板
であり、この振動板6の外周部にはエツジ部材7
を介して上記フレーム5の開口部に支持されてい
る。8は振動板6の下面中央に固定された円筒形
のコイルボビンであり、このコイルボビン8にボ
イスコイル9が巻回され、このボイスコイル9が
前記磁気ギヤツプ部に挿入されている。10はコ
イルボピン8を支持するダンパーである。
FIGS. 1A and 1B show a conventional electrodynamic speaker using a rectangular flat diaphragm. In FIGS. 1A and B, 1 is a yoke with a center pole 2 integrally formed, 3 is an annular magnet fixed on the yoke 1, and 4 is an annular plate fixed on the magnet 3. An annular magnetic gap is formed between the inner peripheral surface of the plate 4 and the outer peripheral surface of the center pole 2. Reference numeral 5 denotes a frame, and the yoke 1 constituting the magnetic circuit is fixed to the inner bottom surface of the frame 5. 6 is a rectangular flat plate diaphragm, and an edge member 7 is provided on the outer periphery of this diaphragm 6.
It is supported by the opening of the frame 5 through the opening of the frame 5. A cylindrical coil bobbin 8 is fixed to the center of the lower surface of the diaphragm 6. A voice coil 9 is wound around the coil bobbin 8, and the voice coil 9 is inserted into the magnetic gap. 10 is a damper that supports the coil bopin 8.

しかしながら、上記従来例のように矩形平板振
動板6の中央を駆動する場合には、振動板6の固
有共振が低い周波数で生じ、スピーカの再生帯域
が非常に狭くなる欠点があつた。
However, when driving the center of the rectangular flat diaphragm 6 as in the conventional example, the natural resonance of the diaphragm 6 occurs at a low frequency, resulting in a drawback that the reproduction band of the speaker becomes extremely narrow.

第2図は上記従来例における振動板の第1次共
振時の振動モードを示しており、この第1次共振
時には、矩形平板振動板6の短辺にほぼ平行な2
本の節線a,a′が生じるものである。このような
振動モードが生じる従来のスピーカにおいては、
第4図のaに示すように、音圧周波数特性におい
て第1次共振周波数f1でピークが生じ音圧平担帯
域が著しく狭くなるものである。
FIG. 2 shows the vibration mode at the time of the first resonance of the diaphragm in the above-mentioned conventional example.
This is where the node lines a and a' of the book occur. In conventional speakers where such vibration modes occur,
As shown in FIG. 4a, a peak occurs at the first resonance frequency f1 in the sound pressure frequency characteristic, and the sound pressure flat band becomes extremely narrow.

本考案は上記従来の欠点を除去するものであ
り、以下に本考案の一実施例について第3図A,
Bとともに説明する。
The present invention eliminates the above-mentioned conventional drawbacks, and an embodiment of the present invention will be described below with reference to FIGS. 3A and 3A.
This will be explained together with B.

本実施例の特徴は、第3図A,Bに示すよう
に、前記従来例における中心駆動により振動板6
の生じる2本の節線a,a′の内の一方の節線a′部
にコイルボビン8を固定し、この節線a′部を駆動
する点にある。
The feature of this embodiment is that, as shown in FIGS. 3A and 3B, the diaphragm 6 is driven by the central drive in the conventional example.
The coil bobbin 8 is fixed to one of the two nodal lines a and a' where the above occurs, and this nodal line a' is driven.

このように、一方の節線部のみを駆動する場合
には、第4図にbで示すように、共振周波数1
おける音圧ピークが実用上問題とならない程度に
小さくでき、高次の共振周波数2まで再生帯域を
拡大できるものである。
In this way, when only one node is driven, the sound pressure peak at resonance frequency 1 can be reduced to an extent that does not pose a practical problem, as shown by b in Figure 4, and the sound pressure peak at resonance frequency 1 can be reduced to an extent that does not pose a practical problem. It is possible to expand the playback band up to 2 .

本考案は上記のように、1個の磁気回路のみを
用い矩形平板振動板を1点駆動する簡単な構成
で、第1次共振周波数における音圧ピークを抑制
し、実用上ほとんど問題のない音圧特性を得るこ
とが可能であり、再生帯域の拡大がはかれるとと
もに、例えば全ての節部分を駆動する多点駆動方
式のスピーカよりも量産性に優れ、低コストなス
ピーカを実現できるという利点を有するものであ
る。
As mentioned above, the present invention has a simple structure in which a rectangular flat diaphragm is driven at one point using only one magnetic circuit, suppresses the sound pressure peak at the first resonance frequency, and produces a sound with almost no practical problems. It has the advantage of being able to obtain high-pressure characteristics, expanding the reproduction band, and being able to realize a speaker that is easier to mass produce and at a lower cost than, for example, a multi-point drive system speaker that drives all nodes. It is something.

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

第1図A,Bは従来の動電型スピーカの上面図
および断面図、第2図A,Bは同スピーカの第1
次共振モードを示す図、第3図A,Bは本考案の
一実施例における動電型スピーカの上面図および
断面図、第4図は従来および本考案の動電型スピ
ーカの音圧周波数特性図である。 1……ヨーク、2……センターポール、3……
マグネツト、4……プレート、5……フレーム、
6……矩形平板振動板、7……エツジ部材、8…
…コイルボビン、9……ボイスコイル、10……
ダンパー。
Figures 1A and B are a top view and a cross-sectional view of a conventional electrodynamic speaker, and Figures 2A and B are the first part of the same speaker.
Figures 3A and 3B are top views and cross-sectional views of an electrodynamic speaker according to an embodiment of the present invention, and Figure 4 is the sound pressure frequency characteristics of the conventional and present electrodynamic speakers. It is a diagram. 1... Yoke, 2... Center pole, 3...
Magnet, 4...Plate, 5...Frame,
6... Rectangular flat plate diaphragm, 7... Edge member, 8...
...Coil bobbin, 9...Voice coil, 10...
damper.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 第1次共振モードの節線が2本であり、かつ矩
形の短辺方向に平行となる矩形平板振動板に、上
記2本の節線の内の一方の節線の中央部にのみ、
1つのコイルボビンを固定し、上記コイルボビン
の駆動により上記矩形平板振動板の第1次共振モ
ードを抑えたことを特徴とする動電型スピーカ。
In a rectangular flat plate diaphragm that has two nodal lines for the first-order resonance mode and is parallel to the short side direction of the rectangle, only at the center of one of the two nodal lines,
An electrodynamic speaker characterized in that one coil bobbin is fixed and the first resonance mode of the rectangular flat plate diaphragm is suppressed by driving the coil bobbin.
JP15665480U 1980-10-31 1980-10-31 Expired JPH0129920Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15665480U JPH0129920Y2 (en) 1980-10-31 1980-10-31

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15665480U JPH0129920Y2 (en) 1980-10-31 1980-10-31

Publications (2)

Publication Number Publication Date
JPS5780995U JPS5780995U (en) 1982-05-19
JPH0129920Y2 true JPH0129920Y2 (en) 1989-09-12

Family

ID=29515800

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15665480U Expired JPH0129920Y2 (en) 1980-10-31 1980-10-31

Country Status (1)

Country Link
JP (1) JPH0129920Y2 (en)

Also Published As

Publication number Publication date
JPS5780995U (en) 1982-05-19

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