JPS59501289A - electromagnetic acoustic transducer - Google Patents
electromagnetic acoustic transducerInfo
- Publication number
- JPS59501289A JPS59501289A JP50212983A JP50212983A JPS59501289A JP S59501289 A JPS59501289 A JP S59501289A JP 50212983 A JP50212983 A JP 50212983A JP 50212983 A JP50212983 A JP 50212983A JP S59501289 A JPS59501289 A JP S59501289A
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- JP
- Japan
- Prior art keywords
- diaphragm
- area
- region
- transducer
- converter
- 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.)
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Classifications
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- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04R—LOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; DEAF-AID SETS; PUBLIC ADDRESS SYSTEMS
- H04R9/00—Transducers of moving-coil, moving-strip, or moving-wire type
- H04R9/02—Details
- H04R9/04—Construction, mounting, or centering of coil
- H04R9/046—Construction
- H04R9/047—Construction in which the windings of the moving coil lay in the same plane
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- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Acoustics & Sound (AREA)
- Signal Processing (AREA)
- Audible-Bandwidth Dynamoelectric Transducers Other Than Pickups (AREA)
- Diaphragms For Electromechanical Transducers (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるため要約のデータは記録されません。 (57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】 鉦I蝕 この発明は拡声器やヘッドホンのような電磁音響変換器に関する。[Detailed description of the invention] gong I eclipse This invention relates to electromagnetic acoustic transducers such as loudspeakers and headphones.
ある種の既知の電磁音響変換器は振動板を備え、その面のうちの1つの上に可聴 周波電流導体を持ち、この導体は振動板を一連の並行な帯に分割し1間隔を置い た並行な電流経路を帯の長平方向の辺に沿って形成する。一連の永久磁石が振動 板と間隔をおいて設けられ、各電流経路に直角な磁場を生み出すように配置され 、それによって、可聴周波電流が導体を流れる間。Certain known electromagnetic acoustic transducers include a diaphragm with an audible It has a frequency current conductor that divides the diaphragm into a series of parallel bands spaced one interval apart. Parallel current paths are formed along the longitudinal sides of the strip. A series of permanent magnets vibrate spaced apart from the plate and arranged to create a magnetic field perpendicular to each current path. , whereby an audio frequency current flows through the conductor.
電流経路を流れる可聴周波電流と磁場との相互作用が駆動力を生み出して振動板 を振動させる。The interaction between the audio frequency current flowing through the current path and the magnetic field creates a driving force that moves the diaphragm. vibrate.
この種の変換器は、振動板の高音域応答が良好な質量が比較的に小さな振動板を 持つ。しかしながら、この種の変換器には。This type of transducer uses a diaphragm with a relatively small mass that provides good high-frequency response. have However, for this type of converter.
振動板の振動を起こす駆動力が振動板の並行な帯の長手方向の辺にのみ加わると いう欠点がある。帯の長さと、帯の長平方向の辺にのみ加わる駆動力とがあいま って、振動板に定在波が生じる。If the driving force that causes the diaphragm to vibrate is applied only to the longitudinal sides of the parallel bands of the diaphragm, There is a drawback. The length of the band does not match the driving force applied only to the long sides of the band. As a result, standing waves are generated on the diaphragm.
振動板に定在波が生しるのは望ましくなく、これを防止するために帯の幅が狭く なるように並行な電流経路を互いの間隔を狭めて配置することが既に提案されて いる。これは変換器の費用の増加を招くので全く申し分がないわけではなく、取 分け。It is undesirable for standing waves to occur on the diaphragm, and to prevent this, the width of the band is narrow. It has already been proposed to arrange parallel current paths with narrower distances from each other so that There is. This is not completely acceptable as it increases the cost of the converter and Separate.
良好な低温域応答を得るために比較的に大きな振動板を備えた変換器の場合に問 題となる。This is a problem for converters with relatively large diaphragms to obtain good low-temperature response. It becomes a problem.
この発明は、上述した欠点を克服あるいは少なくとも軽減する電磁音響変換器を 提供することを目的とする。The present invention provides an electromagnetic acoustic transducer that overcomes or at least alleviates the drawbacks mentioned above. The purpose is to provide.
振動板上に形成された領域に関して本書において用いる場合の「音響的に剛性」 という表現は、その領域が無分割運動を行って(即ち、振動板の領域に定在波を 生じることなく)所定の周波数までの音波を発生するように振動することが出来 ることを意味するものとする。この発明の1形態における電磁音響変換器は、少 なくとも1つの面に可聴周波電流導体を持つ振動板を有し、該導体を波形状パタ ーンに配置することにより振動板を複数の音響的に剛性の領域に分割し且つ領域 の辺に沿って電流経路を形成し、磁石の配列をそれにより発生する磁場が領域の 辺に沿った電流経路と相互作用を行うように配置することにより可聴周波電流が 導体を流れると電流経路に沿って流れる可聴周波電流と個々の磁場との間の相互 作用が振動板の振動を起こす。"Acoustically rigid" as used in this document with respect to areas formed on a diaphragm The expression means that the region is in undivided motion (i.e., it creates a standing wave in the region of the diaphragm). can vibrate to generate sound waves up to a predetermined frequency. shall mean that The electroacoustic transducer in one form of this invention includes a It has a diaphragm with an audio frequency current conductor on at least one surface, and the conductor is arranged in a waveform pattern. divide the diaphragm into multiple acoustically rigid regions and A current path is formed along the edges of the area, and the magnetic field generated by the array of magnets is By arranging it so that it interacts with the current path along the side, the audio frequency current The interaction between an audio current flowing through a conductor and an individual magnetic field along the current path The action causes the diaphragm to vibrate.
波形状パターンは城郭形状あるいは鋸歯状をとりうる。The wavy pattern can be castellated or serrated.
領域は望ましくは長方形である。The region is preferably rectangular.
ある構成においては、振動板は柔軟な材料で、領域は振動板の引っ張りによって 音響的に剛性にすることが出来る。別の構成においては、振動板は柔軟な材料で 、@域は剛性を増す手段を用いて音響的に剛性にすることか出来る。この剛性を 増す手段は例えは、振動板の各領域における。複心曲線のような複合形成物であ る。さらに別の構成においては、振動板は実質的に41性の高い材料で作ること が出来る。In some configurations, the diaphragm is a flexible material and the area is compressed by the tension of the diaphragm. It can be made acoustically rigid. In another configuration, the diaphragm is a flexible material. , @ region can be made acoustically rigid using stiffening means. This rigidity The increasing means are, for example, in each region of the diaphragm. It is a complex formation like a compound curve. Ru. In yet another arrangement, the diaphragm is made of a substantially 41% material. I can do it.
添付図面に示す如き本発明の下記の幾つかの具体的な実施例の説明を参照するこ とにより1本発明の理解はさらに深まるものと思われる。Reference is made to the following description of some specific embodiments of the invention as illustrated in the accompanying drawings. It is believed that this will further deepen the understanding of the present invention.
第1図は、第1の実施例の変換器の斜視図で、詳細が分かり易いように変換器を 部分的に切り取っである。FIG. 1 is a perspective view of the transducer of the first embodiment, with the transducer shown for easy understanding of details. It is partially cut out.
第2図は、第1図の線2−2に沿った断面図で1部分的に切り取っである。FIG. 2 is a cross-sectional view taken along line 2--2 of FIG. 1, with one portion cut away.
第3図は、第1図および第2図の実施例の振動板の代替構造を示す平面図である 。FIG. 3 is a plan view showing an alternative structure of the diaphragm of the embodiment shown in FIGS. 1 and 2; .
第4図は、第1図および第2図の実施例の振動板のさらに別の代替構造を示す平 面図である。FIG. 4 is a flat panel showing yet another alternative construction of the diaphragm of the embodiment of FIGS. 1 and 2; It is a front view.
第5図は、別の実施例の変換器の斜視図で、詳細が分り易いように変換器を部分 的に切り取っである。FIG. 5 is a perspective view of an alternative embodiment of the transducer, with the transducer partially shown for clarity. This is a specific cut.
第6図は、第5図の変換器の振動板の平面図である。6 is a plan view of the diaphragm of the transducer of FIG. 5; FIG.
第7図は、第6図の線7−7に沿った断面図である。FIG. 7 is a cross-sectional view taken along line 7--7 of FIG.
第8図は、第6図の線8−8に沿った断面図である。FIG. 8 is a cross-sectional view taken along line 8--8 of FIG.
第9121は、さらに別の実施例の変換器の振動板と磁石の構成を示す略断面図 である。No. 9121 is a schematic cross-sectional view showing the configuration of a diaphragm and a magnet of a converter according to still another embodiment. It is.
第1O図は、さらに別の実施例の変換器の振動板と磁石の構成を示す略断面図で ある。FIG. 1O is a schematic cross-sectional view showing the structure of the diaphragm and magnet of a converter according to yet another embodiment. be.
第11図は、さらに別の実施例の振動板の支持系を示す略断面図である。FIG. 11 is a schematic cross-sectional view showing a support system for a diaphragm according to yet another embodiment.
添付図面の第1および2図において、第1の実施例の電磁変換器は比較的に質量 が小さい柔軟な振動板11を持ち、この振動板は、単なる一例として、ポリエス テル薄膜、ポリカーボ2−ト薄膜あるいはポリプロピレン薄膜等の多数の薄膜類 のいずれか1紙材料、あるいはアルミニウム等の非磁性体の金属薄膜で形成しつ る。In Figures 1 and 2 of the accompanying drawings, the electromagnetic transducer of the first embodiment has a relatively large mass. has a small flexible diaphragm 11, which diaphragm is made of polyester, by way of example only. A large number of thin films such as polycarbonate thin film, polycarbonate thin film or polypropylene thin film. Formed from one of paper materials or a thin film of non-magnetic metal such as aluminum. Ru.
振動板11は長手方向および横方向に引っ張られており、その外周は剛性の高い 外周枠13に接着あるいは別の方法で固定される。この枠は振動板の各側に、振 動板がその振動中に変位できる空間を形成づ−る。The diaphragm 11 is stretched in the longitudinal and lateral directions, and its outer periphery is made of highly rigid material. It is fixed to the outer peripheral frame 13 by adhesive or other method. This frame is attached to each side of the diaphragm. A space is created in which the moving plate can be displaced during its vibration.
振動板11の1つの面には、城郭形状パターンに構成された可聴周波数電流導体 I5があり1振動板を複数の実質的に長方形の@域17に分割し且つ@域の辺に 沿って電流経路16を形成する。On one side of the diaphragm 11 are audio frequency current conductors arranged in a castellated pattern. There is an I5 that divides one diaphragm into a plurality of substantially rectangular @ areas 17, and on the sides of the @ area A current path 16 is formed along it.
導体を城郭状に構成すると、各領域17 (振動板の外周部の2つ目ごとの領域 を除いて)は各辺に沿った電流経路16を持つ。When the conductor is configured in a castle shape, each area 17 (every second area on the outer periphery of the diaphragm ) has a current path 16 along each side.
振動板のもう一方の面に、導体15と同様な形状を有しそれと180度位相が異 なる別の可聴周波数導体(図示していない)を設けることにより、各外周領域の 最も外側の辺にそって電流の経路を設けることができる。これは、外周領域のそ の他の辺に沿って、そしてその他の領域の各辺に沿って1対の電流経路を設ける 効果がある。費用は増大するが5 この構成によって、外周領域の外側の辺は別 として領域のそれぞれの辺に増大した駆動力が加わるので有益である。外周領域 の外側の辺は振動板の外周に隣接しており、この外周それ自体が外周枠13に固 定されているので、外周領域の外側の辺には増大した駆動力は不要である。The other surface of the diaphragm has a shape similar to that of the conductor 15 and a phase difference of 180 degrees from that of the conductor 15. of each peripheral area by providing another audio frequency conductor (not shown) A current path can be provided along the outermost edge. This is the part of the outer area. a pair of current paths along the other side of the area and along each side of the other area. effective. Although the cost increases5, this configuration allows the outside edges of the peripheral area to be separated. This is advantageous because it applies an increased driving force to each side of the area. outer area The outer side of is adjacent to the outer periphery of the diaphragm, and this outer periphery itself is fixed to the outer peripheral frame 13. Therefore, no increased driving force is required on the outer side of the outer circumferential region.
羊なる一例として、可聴周波導体15はアルミニウムあるいは銅の金属薄膜の形 態をとりうるが、アルミニウムのほうが単位重量当たりの電導率が高いので望ま しい。振動板は、金属薄膜とプラスチック薄膜の積層物のエノチンクによって製 作するか。In one example, the audio conductor 15 is in the form of a thin metal film of aluminum or copper. Aluminum is preferable because it has higher conductivity per unit weight. Yes. The diaphragm is made of Enotink, a laminate of metal thin film and plastic thin film. Do you want to make one?
あるいは金属1腰導体は振動板に印刷、シルク・スクリーンあるいシよ溶着等の 従来技法によって付けうる。別の構成においては、゛導体は振動板に接着された アルミニウムあるいは銅の線の形態をとりうる。振動板が金属薄膜あるいはその 他の電導性材料7)Nら成る場合は、当然ながら導体は振動板から絶縁される。Alternatively, the metal conductor can be printed, silk screened, or welded onto the diaphragm. Can be applied using conventional techniques. In another configuration, the conductor is glued to the diaphragm. It can take the form of aluminum or copper wire. The diaphragm is a thin metal film or In the case of other conductive materials 7) N, the conductor is naturally insulated from the diaphragm.
外周枠13の各0111には、鋼鉄等の磁性体製の音響を通過させる裏当て部材 19がある。各裏当て部材は、外周枠13と一体に成形してもよく、あるいは外 周枠とは別に成形して外周枠に固定してもよい。Each 0111 of the outer frame 13 has a backing member made of a magnetic material such as steel that allows sound to pass through. There are 19. Each backing member may be molded integrally with the outer peripheral frame 13 or It may be molded separately from the peripheral frame and fixed to the peripheral frame.
永久磁石21の配列が各裏当て部材19の振動板11に隣接した側に取りつけら れる。磁石21は一連の段と列に配列され1両配列の各磁石は振動板のそれぞれ の領域17の投影面内に配置される。An array of permanent magnets 21 is attached to the side of each backing member 19 adjacent to the diaphragm 11. It will be done. The magnets 21 are arranged in a series of rows and rows, with each magnet in the array being attached to a respective one of the diaphragms. It is arranged within the projection plane of the region 17.
磁石の形状は角柱で、外面の、即ち、極面23は領域17の形状と幾何学的に類 似する形状であり、この場合は長方形である。各配列の隣接する磁石の極面は互 いに反対の極性であり、それによって隣接する磁石の間に磁場が形成される。The shape of the magnet is a prism, and the outer surface, that is, the pole face 23, is geometrically similar to the shape of the region 17. It has a similar shape, in this case a rectangle. The pole faces of adjacent magnets in each array are mutually of opposite polarity, thereby creating a magnetic field between adjacent magnets.
磁石の極面は、振動板が変位した際に極面に接触することがない程度に、振動板 から離して置かれる。The pole face of the magnet is placed close to the diaphragm to the extent that it does not come into contact with the pole face when the diaphragm is displaced. placed away from
各裏当て部材19は、それに隣接する磁石の面の磁場に磁気抵抗の低い経路をも たらし、磁石の極面23間に存在するそれぞれの磁場を集中する効果がある。こ の効果は、磁場をそれぞれの電流経路16に直角にすることである。Each backing member 19 provides a low reluctance path for the magnetic field of the face of the magnet adjacent to it. This has the effect of concentrating the magnetic fields existing between the pole faces 23 of the magnets. child The effect of is to make the magnetic field perpendicular to the respective current path 16.
本書において既に述べたように、各裏当て部材19は音響を通過させるが1図示 した実施例においては、これは裏当て部材の隣接する磁石の間の区域に穴25を 形成することによって達成される。As mentioned earlier in this document, each backing member 19 allows sound to pass through, but only one In the embodiment shown, this includes holes 25 in the area between adjacent magnets of the backing member. This is achieved by forming.
電流経路16にそって流れる可聴周波電流とそれぞれの磁場との間の相互作用は 、振動板に実質的に圭直な駆動力を各電流経路に与え、これが振動板を振動させ る。従って駆動力は金側に電流経路を持つ領l1i17の各側に加えられる。こ れが、fI4域の音響的に剛性な性質とあいまって、振動板の領域を確実に均一 に無分割運動で振動させる。The interaction between the audio frequency current flowing along the current path 16 and the respective magnetic field is , a substantially direct driving force is applied to each current path on the diaphragm, which causes the diaphragm to vibrate. Ru. Therefore, driving force is applied to each side of region l1i17 with the current path on the gold side. child This, combined with the acoustically rigid nature of the fI4 region, ensures that the area of the diaphragm is uniform. vibrate in undivided motion.
図面の第3づよび4図は、振動板上の可聴周波数電流導体の構成の変形を示し、 これら二図面の参照番号は第1および2図の実施例に関して説明したものと同じ 部分を示す。第3図に示した構造においては、導体は鋸歯状パターンに配置され 、振動板11を複数の実質的に長方形の領域17に分割する。第4図に示す構造 においては、導体15は鋸歯状パターンに配置され、振動板11を複数の実質的 に三角形の領域に分割する。この構成においては、磁石21の極面(点線で示す )の形状は三角形の領域の形状と幾何学的に類似する。Figures 3 and 4 of the drawings show variations in the arrangement of audio frequency current conductors on the diaphragm; The reference numbers in these two figures are the same as those described with respect to the embodiment in figures 1 and 2. Show parts. In the structure shown in Figure 3, the conductors are arranged in a sawtooth pattern. , dividing the diaphragm 11 into a plurality of substantially rectangular regions 17 . Structure shown in Figure 4 , the conductors 15 are arranged in a sawtooth pattern to connect the diaphragm 11 to a plurality of substantially Divide into triangular regions. In this configuration, the polar face of the magnet 21 (indicated by a dotted line) ) is geometrically similar to the shape of the triangular region.
次に、添付図面の第5.6.7および8図に、各面に可聴周波導体115(分か り易いように第5図においては振動板の下面例の導体は省略しである)を持つ振 動板111を備えた電磁音響変換器を示す。可聴周波数導体115aおよび11 5bは振動板上に城郭形状パターンに配置され、振動板を複数の実質的に長方形 の領域117に分割し且つ領域の辺に沿って電流経路116を形成する。導体1 15a23よび115bは互いに類似する形状であるが位相が180度異l9( 図面の第6図が一番分り易い)、それによって少なくとも1つの導体経路116 が各領域の各辺に沿う。実際。Next, Figures 5.6.7 and 8 of the accompanying drawings show an audio frequency conductor 115 (separated) on each side. For ease of illustration, the conductor on the bottom of the diaphragm is omitted in Figure 5). An electroacoustic transducer with a moving plate 111 is shown. Audio frequency conductors 115a and 11 5b are arranged in a castellated pattern on the diaphragm, and the diaphragm is arranged in a plurality of substantially rectangular shapes. The current path 116 is divided into regions 117 and current paths 116 are formed along the sides of the regions. Conductor 1 15a23 and 115b have similar shapes to each other, but their phases differ by 180 degrees l9( 6 of the drawings), whereby at least one conductor path 116 along each side of each region. actual.
振動板の外周部の領域は別として、全ての領域の各辺にそって1対の電流経路が もたらされる。導体115aおよび115bは振動板トに別の過当なパターン、 例えば鋸歯状パターンに配置しうろことを理解すべきである。しかしながら、領 域117は実質的に伎す一形の形状であることが望ましい。さらに、必要であれ ば(第1および2図の実施例のように)、振動板に導体を1つだけ画人うること も理解すべきである。A pair of current paths runs along each side of all areas, apart from the outer peripheral area of the diaphragm. brought about. The conductors 115a and 115b are arranged on the diaphragm in a different pattern, For example, it should be understood that the scales are arranged in a serrated pattern. However, territory Preferably, area 117 is substantially curved in shape. Furthermore, if necessary If (as in the embodiments of Figures 1 and 2) there is only one conductor on the diaphragm. should also be understood.
振動板111は柔軟な薄板材料から形成され、@域117に剛性を商める手段1 18を備え”CH域を音響的に剛性なものとする。The diaphragm 111 is formed from a flexible thin plate material, and means 1 for imparting rigidity to the region 117 18 to make the CH region acoustically rigid.
図示した構成においては、剛性を高める手段118は、それぞれ0)領域で振動 板に形成された複合形成物から成る。特に1図示した構成においては、複合形成 物はそれぞれ半球ドームの形状であり、各ドームはそれぞれの領域の外周あるい はその近辺で長方形の基板と一体になる。別の構造においては、複合形成物は、 長方形の基板と一体となった中空の円錐、あるいは長方形の底面を持つ中空の四 角錐であってもよい。In the configuration shown, the stiffening means 118 each have vibrations in the 0) region. Consists of a composite formation formed into a plate. In particular, in the configuration shown in Figure 1, the composite formation Each object has the shape of a hemispherical dome, and each dome is the outer circumference or is integrated with the rectangular substrate in the vicinity. In another construction, the composite formation is A hollow cone integrated with a rectangular substrate or a hollow square with a rectangular base. It may also be a pyramid.
(辰勅板111は、ポリエステルあるいはポリカーボネート等の過当なプラスチ ック材料、銅合金等の金属、あるいは複合材料で製作することが出来る。振動板 litには、真空成形、射出成形、あるいは圧縮成形等の適当な技法によって複 合形成物118を形成することが出来る。(The dragon plate 111 is made of excessive plastic such as polyester or polycarbonate. It can be manufactured from metals such as copper alloys, or composite materials. diaphragm The lit can be manufactured using suitable techniques such as vacuum forming, injection molding, or compression molding. A composite object 118 can be formed.
振動板111はその外周で懸垂系120によって支持され、この懸垂糸はS@板 の面に実質的に歩直な方向に振動板が振動することを妨げない。図示した実施例 においては、懸垂系は振動板と一体に形成され外周枠113に固定される。別の 構成においては、懸垂糸は振動板とは別に形成して、振動板はその外周で懸垂糸 に接合あるいはその他の方法で固定することも出来る。The diaphragm 111 is supported on its outer periphery by a suspension system 120, and this suspension string is connected to the S@plate. does not prevent the diaphragm from vibrating in a direction substantially perpendicular to the plane of the diaphragm. Illustrated embodiment In this case, the suspension system is formed integrally with the diaphragm and fixed to the outer peripheral frame 113. another In the configuration, the suspension strings are formed separately from the diaphragm, and the diaphragm has the suspension strings formed on its outer periphery. It can also be fixed by bonding or other methods.
振動板111の複合形成物118の突き出した側と反対側に、振動板に間隔を保 って、鋼等の磁性体材料で出来た音響を通過させる裏当て部材119が置かれる 。裏当て部材119は外周枠113と一体にあるいは別々に形成することが出来 る。On the opposite side of the diaphragm 111 from the protruding side of the composite formation 118, a spacer is provided on the diaphragm 111 to maintain a gap. Therefore, a backing member 119 made of a magnetic material such as steel that allows sound to pass through is placed. . The backing member 119 can be formed integrally with the outer frame 113 or separately. Ru.
永久磁石121の配列が裏当て部材119の振動板111に面した側に取りつけ られる。これまでに述べた実&i例と同様に、磁石121 は一連の段と列とに 配置され、各磁石はそれぞれの珀h3i 117の投影面内に置かれ、隣接する 磁石の極面はりいに異なる極性である。磁石121の形状は角柱で、極面123 の形状は@域117の形状と幾何学的に類似する。An array of permanent magnets 121 is attached to the side of the backing member 119 facing the diaphragm 111. It will be done. As in the previous examples, the magnets 121 are arranged in a series of rows and rows. arranged, each magnet is placed within the projection plane of each square h3i 117, and the adjacent The polar faces of the magnets have very different polarities. The shape of the magnet 121 is a prism, and the pole face 123 The shape of is geometrically similar to the shape of @ area 117.
裏当て部材は、そn、に隣接する磁石の面において磁場に磁気抵抗の低い経路を もたらし、極面間に存在する磁場を集中する効果かある。この効果は、vi、場 をそれぞれの電流経路に直角にすることである。The backing member provides a path of low reluctance to the magnetic field on the surface of the magnet adjacent to the backing member. This has the effect of concentrating the magnetic field that exists between the pole faces. This effect is vi, field is perpendicular to each current path.
この実施例の変換器は、これまで述べた実施例といくらか類似する要領で機能す るか、@域117の音響的な剛性は、振動板の引っ張りによらず複合形成物11 8によって保持される。The transducer of this embodiment functions in a somewhat similar manner to the previously described embodiments. In other words, the acoustic rigidity of @ region 117 is independent of the tension of the diaphragm, and is independent of the composite structure 11. 8.
第9,10および11図に示した実施例の変換器は、第5から8図までに図示し た変換器とある程度類似しており、第9,10および11図に用いた参照番号は 第5から8図までの実施例に関して説明したものと同じ部分を示す。The transducers of the embodiments shown in Figures 9, 10 and 11 are illustrated in Figures 5 through 8. The reference numbers used in Figures 9, 10 and 11 are The same parts as described with respect to the embodiments of FIGS. 5 to 8 are shown.
第9図において1図示した変換器は、第5から8図までのものと、振動板の一面 だけに可聴周波数導体115があること、および導体が縁部で振動板111に接 着されたリボンの形状である点で異なる。このリボンにより形成されるそれぞれ の電流経路116は、永久磁石121の極面−ヒに取りつけた隣接する極片12 4間の区域122内に位置する。この構成において、振動板111は。The transducer shown in one diagram in Figure 9 is the one shown in Figures 5 to 8, and one side of the diaphragm. that there is an audio frequency conductor 115 only at the edge and that the conductor contacts the diaphragm 111 at the edge The difference lies in the shape of the ribbon worn. Each formed by this ribbon The current path 116 is connected to the adjacent pole piece 12 attached to the pole face A of the permanent magnet 121. It is located within the area 122 between 4 and 4. In this configuration, the diaphragm 111 is.
導体が磁場の影響から逃れることなく、比較的大きな変位をすることが可能であ る。リボンは横方向の剛性を高めるためにその俗手万同に沿って曲げうる。It is possible for a conductor to undergo a relatively large displacement without escaping the influence of the magnetic field. Ru. The ribbon can be bent along its length to increase lateral stiffness.
代替の構成において、リボン115は振動板の平面から外開きに突き出た取りつ け台に接着あるいは別の方法で固定することも出来る。In an alternative configuration, the ribbon 115 is a mount that projects outwardly from the plane of the diaphragm. It can also be glued or otherwise fixed to the stand.
第10図に示す構成においては、永久磁石121は−っ置きの領域117aだけ の投影面内に設けられ、その他の領域117bの投影面に;ま裏当て部材119 と一体のあるいはそれと接触した極片126がある。永久磁石121はそれらの 極面が1.1lffi性となるように配置され、且つそれぞれには極片124が 取りつけである。磁場は隣接J−る極片124 と126との間に存在し、この 構成では各領域117に対応1−る永久磁石を不要にする。In the configuration shown in FIG. The backing member 119 is provided in the projection plane of the other region 117b; There is a pole piece 126 integral with or in contact with. The permanent magnet 121 The pole faces are arranged to have a 1.1lffi property, and each pole piece 124 is provided. It's a fixture. A magnetic field exists between adjacent pole pieces 124 and 126; The configuration eliminates the need for permanent magnets corresponding to each region 117.
第11図には、振動板111を支持するための代替の構成を示す。An alternative arrangement for supporting diaphragm 111 is shown in FIG.
振動板はその外周部で支持されるのではなく、その内側で複数の弾性支持部材1 29によって支持される。弾性の支持部材129は、振動板中の剛性を高める複 数の形成部118のそれぞれの頂点131 と、振動板から離して取りつけた4 り性の高い部材133との間に取りつけられる。この形態の支持系を用いると、 隣接する@域117が互いに限られた角運動をすることが可能な振動板を用いる ことが可能となる。The diaphragm is not supported by its outer circumference, but by a plurality of elastic support members 1 inside it. Supported by 29. The elastic support member 129 is a composite material that increases the rigidity in the diaphragm. Each vertex 131 of the number forming part 118 and the 4 It is attached between the member 133 and the highly resilient member 133. With this form of support system, Using a diaphragm that allows adjacent @ regions 117 to make limited angular movements with respect to each other becomes possible.
さらに別の実施例(図示していない)において、振動板は剛性の高い材料で形成 することが出来る。この構成においては。In yet another embodiment (not shown), the diaphragm is formed of a rigid material. You can. In this configuration.
振動板は、第5から8図の実施例に用いられたものと類似する外IfI部慈老糸 によるか、あるいは第11図の実施例に用いられたものと類似する懸垂糸によっ て支持することが出来る。The diaphragm has an outer IfI section similar to that used in the embodiments of Figures 5 to 8. or by a suspension string similar to that used in the embodiment of FIG. It can be supported by
この発明の範囲はごこに記述した実施例の範囲に限定されるものではないこと、 且つこの発明の精神から離れることなく種々の変史あるいは変形を行いうること を理解すべきである。that the scope of this invention is not limited to the scope of the embodiments described herein; Moreover, various changes or modifications can be made without departing from the spirit of this invention. should be understood.
IG I IG 2 日G3 IG 5 FIG 6 FIG 9 lG10 国際調査報告 InIIIfIIa+101+1^””II””0PCT/AIJ!+3/′0 0084第1頁の続き 優先権主張 @1982年9月13日■オーストラリア(AU)■PF5845 ■1982年11月19日■オーストラリア(AU)■PF6877IG I IG 2 Japan G3 IG 5 FIG 6 FIG 9 lG10 international search report InIIIfIIa+101+1^””II””0PCT/AIJ! +3/'0 0084 Continuation of page 1 Priority claim @ September 13, 1982 ■ Australia (AU) ■ PF5845 ■November 19, 1982 ■Australia (AU) ■PF6877
Claims (1)
Applications Claiming Priority (6)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
AUPF492482 | 1982-07-19 | ||
AU5845FREGB | 1982-09-13 | ||
AUPF584582 | 1982-09-13 | ||
AU4924FREGB | 1982-11-19 | ||
AUPF687782 | 1982-11-19 | ||
AU6877FREGB | 1982-11-19 |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS59501289A true JPS59501289A (en) | 1984-07-19 |
Family
ID=27157158
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP50212983A Pending JPS59501289A (en) | 1982-07-19 | 1983-06-27 | electromagnetic acoustic transducer |
Country Status (3)
Country | Link |
---|---|
EP (1) | EP0113732A4 (en) |
JP (1) | JPS59501289A (en) |
WO (1) | WO1984000460A1 (en) |
Cited By (3)
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JP2003102088A (en) * | 2001-09-19 | 2003-04-04 | Fps:Kk | Planar acoustic transducer |
JP2006050665A (en) * | 2002-05-02 | 2006-02-16 | Harman Internatl Industries Inc | Electrodynamic type planar loudspeaker |
JP2010245601A (en) * | 2009-04-01 | 2010-10-28 | Foster Electric Co Ltd | Complete drive loudspeaker |
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EP0206458B1 (en) * | 1985-04-17 | 1992-07-01 | Geoquip Security Systems Limited | Vibration-sensitive transducer |
EP0493450A4 (en) * | 1989-09-22 | 1993-05-12 | Antony Leonard Trufitt | Planar speakers |
GB2248006A (en) * | 1990-04-25 | 1992-03-18 | Haqi Ismail Hussain Almossawi | A responsive robotic technique |
US5430805A (en) * | 1990-12-27 | 1995-07-04 | Chain Reactions, Inc. | Planar electromagnetic transducer |
FR2687035A1 (en) * | 1992-02-05 | 1993-08-06 | Navarron Jean Pierre | Device for sound reproduction by movement of a layer of air |
GB2265519A (en) * | 1992-03-19 | 1993-09-29 | Jonathan Neil Smith | Flat monopole loudspeaker |
US5627903A (en) * | 1993-10-06 | 1997-05-06 | Chain Reactions, Inc. | Variable geometry electromagnetic transducer |
KR100352859B1 (en) * | 1997-07-09 | 2002-09-16 | 에프피에스 인코포레이티드 | Planar acoustic transducer |
US6104825A (en) * | 1997-08-27 | 2000-08-15 | Eminent Technology Incorporated | Planar magnetic transducer with distortion compensating diaphragm |
JPWO2003073787A1 (en) * | 2002-02-28 | 2005-06-23 | 古河電気工業株式会社 | Flat speaker |
EP2033480B1 (en) | 2006-05-22 | 2012-07-11 | Audio Pixels Ltd. | Volume and tone control in direct digital speakers |
US8457338B2 (en) | 2006-05-22 | 2013-06-04 | Audio Pixels Ltd. | Apparatus and methods for generating pressure waves |
WO2007135678A2 (en) | 2006-05-22 | 2007-11-29 | Audio Pixels Ltd. | Direct digital speaker apparatus having a desired directivity pattern |
GB2443228B (en) * | 2006-10-25 | 2010-02-10 | Gary Paul Nicholson | Piezo-electric loudspeaker |
EP2846557B1 (en) | 2007-11-21 | 2019-04-10 | Audio Pixels Ltd. | Improved speaker apparatus |
US9391541B2 (en) | 2010-03-11 | 2016-07-12 | Audio Pixels Ltd. | Electrostatic parallel plate actuators whose moving elements are driven only by electrostatic force and methods useful in conjunction therewith |
DK2643982T3 (en) | 2010-11-26 | 2022-07-04 | Audio Pixels Ltd | DEVICE FOR GENERATING A PHYSICAL MEASUREMENT POWER AND METHOD OF MANUFACTURING THE DEVICE |
US9880533B2 (en) | 2012-05-25 | 2018-01-30 | Audio Pixels Ltd. | System, a method and a computer program product for controlling a group of actuator arrays for producing a physical effect |
WO2013175477A1 (en) | 2012-05-25 | 2013-11-28 | Audio Pixels Ltd. | A system, a method and a computer program product for controlling a set of actuator elements |
KR20170137810A (en) | 2015-04-15 | 2017-12-13 | 오디오 픽셀즈 리미티드 | Method and system for detecting at least the position of an object in space |
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FR1329295A (en) * | 1962-07-19 | 1963-06-07 | Philips Nv | Electro-dynamic magnetic system |
NL6613713A (en) * | 1966-09-29 | 1968-04-01 | ||
US3873784A (en) * | 1973-03-29 | 1975-03-25 | Audio Arts Inc | Acoustic transducer |
AT325694B (en) * | 1973-09-14 | 1975-11-10 | Akg Akustische Kino Geraete | ELECTRODYNAMIC CONVERTER, IN PARTICULAR SOUND CONVERTER |
DE2461258C3 (en) * | 1974-12-23 | 1978-09-07 | Foster Electric Co., Ltd., Tokio | Diaphragm for an electroacoustic transducer |
GB1471297A (en) * | 1974-12-23 | 1977-04-21 | Foster Electric Co Ltd | Electrodynamic type electroacoustic transducer |
US4337379A (en) * | 1979-01-16 | 1982-06-29 | Nippon Gakki Seizo Kabushiki Kaisha | Planar electrodynamic electroacoustic transducer |
US4210786A (en) * | 1979-01-24 | 1980-07-01 | Magnepan, Incorporated | Magnetic field structure for planar speaker |
FR2450020A1 (en) * | 1979-02-20 | 1980-09-19 | Soria Jean Yves | Loudspeaker with several electrodynamic driving units - which fit over membrane to apply uniform force to latter |
NL7908447A (en) * | 1979-11-20 | 1981-06-16 | Philips Nv | MAGNETIC SYSTEM FOR AN ELECTROACOUSTIC CONVERTER. |
FR2477821A1 (en) * | 1980-03-06 | 1981-09-11 | 3A Art Acoustique Appliquee Sa | ELECTRODYNAMIC SPEAKER |
US4544805A (en) * | 1981-09-25 | 1985-10-01 | Tadashi Sawafuji | Plane speaker |
-
1983
- 1983-06-27 EP EP19830901888 patent/EP0113732A4/en not_active Withdrawn
- 1983-06-27 WO PCT/AU1983/000084 patent/WO1984000460A1/en not_active Application Discontinuation
- 1983-06-27 JP JP50212983A patent/JPS59501289A/en active Pending
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2003102088A (en) * | 2001-09-19 | 2003-04-04 | Fps:Kk | Planar acoustic transducer |
JP4588944B2 (en) * | 2001-09-19 | 2010-12-01 | 株式会社エフ・ピー・エス | Planar acoustic transducer |
JP2006050665A (en) * | 2002-05-02 | 2006-02-16 | Harman Internatl Industries Inc | Electrodynamic type planar loudspeaker |
JP2006054917A (en) * | 2002-05-02 | 2006-02-23 | Harman Internatl Industries Inc | Electrodynamic type planar loudspeaker |
JP4713285B2 (en) * | 2002-05-02 | 2011-06-29 | ハーマン インターナショナル インダストリーズ インコーポレイテッド | Electrodynamic planar loudspeaker |
JP2010245601A (en) * | 2009-04-01 | 2010-10-28 | Foster Electric Co Ltd | Complete drive loudspeaker |
Also Published As
Publication number | Publication date |
---|---|
WO1984000460A1 (en) | 1984-02-02 |
EP0113732A4 (en) | 1986-02-13 |
EP0113732A1 (en) | 1984-07-25 |
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