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WO1981002501A1 - Magnetic circuit for an electro-mechanical transducer of a dynamic electricity-type - Google Patents

Magnetic circuit for an electro-mechanical transducer of a dynamic electricity-type Download PDF

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Publication number
WO1981002501A1
WO1981002501A1 PCT/JP1981/000035 JP8100035W WO8102501A1 WO 1981002501 A1 WO1981002501 A1 WO 1981002501A1 JP 8100035 W JP8100035 W JP 8100035W WO 8102501 A1 WO8102501 A1 WO 8102501A1
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Prior art keywords
magnetic pole
magnetic field
magnetic
coil
conductor
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PCT/JP1981/000035
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French (fr)
Japanese (ja)
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K Sakai
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Classifications

    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04RLOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; DEAF-AID SETS; PUBLIC ADDRESS SYSTEMS
    • H04R9/00Transducers of moving-coil, moving-strip, or moving-wire type
    • H04R9/02Details
    • H04R9/025Magnetic circuit
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04RLOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; DEAF-AID SETS; PUBLIC ADDRESS SYSTEMS
    • H04R9/00Transducers of moving-coil, moving-strip, or moving-wire type
    • H04R9/02Details
    • H04R9/04Construction, mounting, or centering of coil
    • H04R9/041Centering
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04RLOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; DEAF-AID SETS; PUBLIC ADDRESS SYSTEMS
    • H04R9/00Transducers of moving-coil, moving-strip, or moving-wire type
    • H04R9/02Details
    • H04R9/04Construction, mounting, or centering of coil
    • H04R9/046Construction
    • H04R9/047Construction in which the windings of the moving coil lay in the same plane
    • H04R9/048Construction in which the windings of the moving coil lay in the same plane of the ribbon type

Definitions

  • a method of driving a loudspeaker for a relatively versatile production machine will be described.
  • Each of the following two forms will be described, which are roughly classified into those using a conductor in a shape 10 and those using a ribbon or a leaf-like conductor.
  • a compensating coil (11) is provided in an air gap (3) to positively cancel a cross magnetic field (8) generated by a movable coil (6).
  • a current for canceling the cross magnetic field (8) is passed through the metal (11), and the characteristics can be improved with an extreme increase in the material used.
  • the current flowing through the compensation coil (11) is obtained by amplifying the shape of the signal current supplied to the movable coil (6) by another amplifier or by passing the signal current through a transformer.
  • the simplest method is to connect a movable coil (6) and a compensation coil (11) in series considering the polarity and treat both ends as input terminals for the speed. It is good.
  • the fertility to be improved not only the apparent distortion of the sound output is improved, but also the phase characteristics of the output waveform, particularly the rising characteristics of the 3 ⁇ 4 shape in the low frequency range are remarkably improved.
  • Fig. 4 shows the source of a speaker using a ribbon or leaf-shaped conductor.
  • the gap (14) formed by the opposing magnetic poles (12) and (13) has a magnetic field line C15).
  • the movable conductor (17) supported at both ends by moving it in the direction of arrow (16) so that it has flexibility as a whole or only at both ends. I do.
  • a signal current flows through the movable conductor (17)
  • a repulsive force generated between the movable conductor (17) and the magnetic field line (15) generates a driving force in the direction of the arrow [16] on the movable conductor ( 17 ) and moves.
  • the original magnetic field is disturbed as shown in Fig. 5 due to the cross magnetic field (18) generated around (). This results in having the coiled conductor
  • the characteristics can be improved by passing the other current.
  • the one using the movable coil (6) is in contact with the air gap (3) of the center magnetic pole (1) and / or the outer magnetic pole (2) as shown in Fig. 7.
  • Casting (20), (21) is provided along the surface, and a compensation coil (11) is buried in it, and a ribbon-shaped or leaf-shaped movable conductor (17) is used.
  • grooves (22) and (23) are formed along the conductor (17) on the surface of the opposing magnetic poles (12) and (13) in contact with the air gap (14).
  • the compensation conductor (19) is embedded in it.
  • FIG. 9 is a vertical cross-sectional view of a dynamic loud-speech force embodying the present invention D, which is compensated for in the air gap (24) along the surfaces of the center pole (25) and the outer pole (26).
  • This is the same as general loud-speaking force except that coils (27) and [28] are fixed.
  • the compensation coils (27) and (28) have the same winding density as the movable coil (29), that is, the same number of turns as the unit length in the axial direction of the movable coil (29).
  • the compensation coil is divided into two as shown in the figure, the total number will be the total number, and the length will be roughly the same as the length of the movable coil (29) or in the gap (24)
  • the range is the same length as the effective length of the magnetic field.
  • the direction of the crossing magnetic field generated by each coil when a common current flows through the movable coil (29) and the compensation coil (27), [28] is read as shown in Fig. 10. It is connected in series so that it is reversed.
  • V IPO (2) When using a ribbon-shaped or leaf-shaped conductor
  • FIG. 11 is a two-sided view of the soot force implementing the present invention.
  • FIG. 11 shows the magnetic poles (3Q) and (31)] formed in the gap (32) formed parallel to the movable conductor (33). This is the same as the conventional spin force except that the compensating conductor (34) is provided so as to sandwich it.
  • the compensating conductor (34) and the crossing magnetic field generated by the movable conductor are arranged so that the signal current flowing in the movable conductor (33) turns back and flows in the opposite direction. Connected so that it is upside down.
  • the gaps between the magnetic poles (25) and (26) are shown in Fig. 12 in order to prevent a decrease in efficiency due to an increase in the gap size for providing a compensation coil or compensation conductor.
  • Grooves (35) and (36) are provided on the surface in contact with [24] along the winding direction of the movable coil (29), and compensation coils (27) and (28) are embedded in them. By doing so, the increase in the size of the gap (24) can be reduced, and a decrease in efficiency can be prevented.
  • a groove is formed along the movable conductor (33) on the surface of the magnetic poles (30), (31) in contact with the gap (32). (37) is provided, and the compensating conductor (34) is embedded in it.
  • FIG. 1 9 Up to Fig. 8 is for explanation of "Disclosure of invention", Fig. 9! ) Figures up to Fig. 12 are drawings for explaining "the best mode for carrying out the invention".
  • Fig. 1 is a drawing showing the generation of a crossing magnetic field in a radiating beaker using a coil-shaped conductor. It is a drawing provided with a compensation coil for canceling.
  • Fig. 4 is a drawing showing the generation of a crossover magnetic field by the speed using a ribbon or a leaf-shaped conductor.
  • Fig. 5 is a drawing showing the state where the magnetic field lines are disturbed by the crossing magnetic field. Is a drawing provided with a compensating conductor for canceling the cross magnetic field.
  • FIG. 7 is a drawing showing an example in which a compensation coil is embedded
  • FIG. 8 is a drawing showing an example in which a compensation conductor is embedded in a groove provided on each magnetic pole surface.
  • FIG. 9 and FIG. 10 are drawings showing an example in which the present invention is applied to a Loudsby force using a coil-shaped conductor.
  • FIG. 11 is a diagram showing an example in which the present invention is applied to a speaker using a ribbon-shaped or leaf-shaped conductor.
  • FIG. 12 is a drawing showing an example in which the compensation coil is stored
  • FIG. 13 is an example in which the compensation conductor is stored in grooves provided on the surface of the magnetic pole.

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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)
  • Circuit For Audible Band Transducer (AREA)

Abstract

Generally, an electro-mechanical transducer of a dynamic electric type, typified by the operational principle of a loudspeaker, or microphone, or the crossing magnetic field produced when a moving coil (29) or a moving conductor (33) is supplied with signal current disturbs the magnetic field within magnetic gaps (24, 32), causing distortions in the output thereof. A magnetic circuit for an electro-mechanical transducer of a dynamic electric type, is provided for correcting the above-mentioned distortions, in which compensating coils (27, 28) or compensating conductors (34) are provided within the magnetic gaps (24, 32) or grooves (35, 36, 37) formed in the surface of magnetic poles (25, 26, 30, 31). The compensating coils (27, 28) or conductors (34) are supplied with a current corresponding to the signal current so as to produce a crossing magnetic field counter to the crossing field produced by the moving coil (29) or the moving conductor (33) supplied with the signal current, so that disturbances in the magnetic field within the magnetic gaps (24, 32) are prevented.

Description

Figure imgf000003_0001
Figure imgf000003_0001

中に電流 流れることによ!)原磁界の磁ガ鎳分布 乱れ'を生じ、.. 10そのため発生する電磁斥力或いは電磁起電力に歪を '生ずる 本 :発 . 明はその ¾カ線分布の乱れを減少せしめ、 しかして 力 おける 歪を改善 ;せんとするものである。 By flowing current inside! ) 'Cause, .. 10 electromagnetic repulsion or distortion to the electromagnetic electromotive force generated because the'磁Ga鎳distribution disturbance of the original magnetic field caused present:. Inventions are made to reduce the disturbance of the ¾ mosquito line distribution, Thus the force Improve the distortion in the picture ;

背 景 技 銜  Background technique

Figure imgf000003_0002
, - '. ¾ ^!? ス ピー カ - ©磁気回路入門 - - 3 ) ^用'新案出願公告. 昭 4 4 - 8 0 4 0
Figure imgf000003_0002
,-'. ¾ ^! ? Speaker-© Introduction to Magnetic Circuits--3) Notice of application for new model for ^.

' 、 ' 考案の名称 ス ピーカ— . ',' Name of the device Speaker.

4 ) 特許出願公告 昭 5 1 — 8 5 6 9  4) Patent application public announcement 5 1 — 8 5 6 9

5 発明の名称 · 磁気回路 : - : 5 Title of Invention · Magnetic Circuit : - :

' 発 明 の 開 示  '' Disclosure of the invention

発明を実施した例として生産数の比較的多 才—ディ ォ用のラ ウ ドス ピ -カの駆動方式につ て説明するが、 その方式に於 て 更に駆動される導体の形状の相違でコィル状導体を使用したもの 10 と、 リ ボン又はリ ーフ状導体を使用したものとに大別される故夫 々 の形態に就いて説明する。  As an example of implementing the invention, a method of driving a loudspeaker for a relatively versatile production machine will be described. Each of the following two forms will be described, which are roughly classified into those using a conductor in a shape 10 and those using a ribbon or a leaf-like conductor.

第 1 図に於いて中心磁極 (1)と外周磁極 (2)によ 形成された空隙 (3)には両磁極間に通じる磁力線 (4)によるほ ^平等な磁界:^存在し ' てお ]) 、 該空隙 (3)内にボビン (5)に巻かれた可動コ (6)がその中 15 心軸つま り矢印 (7)の方向にのみ違動出来るよ う支持されている。 ノ 可 ¾: ^ ル (6)に信号電流が流れるこ とによ 磁力線 (4)と ^動コ ィル (6) £ S f に発生する斥力が駆動力と Ϊ)可勣コィル (6)は矢印 ( の画か ている方向に前後運動し、 その違勣がボビンの先端に 取付けられるサウ ン ドラジェ—タを振動させることによ 電気工 20 ネ ルギ -が音響に変換されるのである。 この場合変換された音響 ; ■ m力の ¾形が信号電流の波形に対して歪を少¾ く保たれるため : ' 、 可動コィ ル (6)に作用する駆動力が信号電流の波形の大きさ ' 比例し ¾ければ らずそのためには空隙 (3)内に於ける ¾力線 (4)  In Fig. 1, the air gap (3) formed by the central magnetic pole (1) and the outer magnetic pole (2) has a nearly equal magnetic field due to the lines of magnetic force (4) passing between the magnetic poles. ]), The movable core (6) wound around the bobbin (5) in the space (3) is supported so that it can move only in the direction of the 15-axis shaft, that is, the direction of the arrow (7). ¾: The repulsive force generated in the magnetic field line (4) and the dynamic coil (6) due to the signal current flowing in the coil (6) and the driving force (6) Moves back and forth in the direction of the arrow (), and the conversion causes the sound engineer attached to the tip of the bobbin to vibrate, which converts the electrician 20 energies into sound. In this case, the converted sound; ■ The shape of the m force keeps the distortion of the signal current waveform small: 'The driving force acting on the movable coil (6) changes the waveform of the signal current. The size 'must be proportional, and for that purpose the force line in the air gap (3) (4)

' 分布が均一、 つま 平等磁界であることが要求される。 該磁力線 25 (4)の均一化の めに中心磁極 (1)および外局磁極 (2)の形状は勿論の  '' It is required that the distribution is uniform, that is, a uniform magnetic field. The shape of the central magnetic pole (1) and the external magnetic pole (2) are of course

O?,:PI VIPO こと、 両磁極 (1) , (2)の空隙 (3)に接する部分の材贊 ; 力線の飽和 度等諸種の条件を考慮して設計されるのが通例でぁ が、. 実際に 可動コィル (6)に作用する駆動力の変化波形に歪を生じ最終的に音 響出力に歪を発生する原因の一部と して、 信号電流による磁界の 5歪が大き ¾ フ ァ ク タ一 と して考え られる。 O?,: PI VIPO , Magnetic poles (1), (2) a gap (3) to the contact portion of the wood 贊;. The is designed in consideration of the conditions of saturation, etc. Shoshu field line but § customary, actually moving As one of the causes of the distortion of the change waveform of the driving force acting on the coil (6) and finally the distortion of the sound output, 5 distortion of the magnetic field due to the signal current is large. It is considered as.

信号電流が可動コ イ ル (6)に流れると既存の磁力線 (4)とは別に信 When a signal current flows through the movable coil (6), the signal is separated from the existing magnetic field lines (4).

- 号電流による新た 磁力籙、 通称交叉磁界 (8)が発生する。 今、 あ る瞬間交叉磁界 (8)の向きが矢印 (9)の方向と仮定すると、 既存の磁 力線 (4)を歪ませる結杲第 2 図に示すよ うに磁力線 (4)の分布に歪を-A new magnetic force に よ る, commonly known as a cross magnetic field (8), is generated by the signal current. Now, assuming that the direction of the instantaneous cross magnetic field (8) is in the direction of the arrow (9), the distribution of the magnetic field lines (4) is distorted as shown in Fig. 2, which distorts the existing magnetic field lines (4). Distortion

10 生ずる。 一応の理論と してはこの歪んだ磁力線 (4)が元の形状に戻 ろう と し、 その力が可動コ イ ル (6)に対し矢印(10)方向えの駆動力 とるつて作用するのであるカ 、 その際の可勣コィ ル (6)の進行方向 は磁力線 (4)の密度がも との平等磁界の時よ D粗に ってお D、 信 号電流から可動コィル (6)に伝違されるェネルギ -が平等磁界の時10 Occurs. As a prima facie theory, this distorted line of magnetic force (4) tends to return to its original shape, and this force acts on the movable coil (6) as a driving force in the direction of the arrow (10). At a certain point, the traveling direction of the movable coil (6) is coarser than when the density of the lines of magnetic force (4) is the same as the original magnetic field, and the moving direction of the movable coil (6) changes from the signal current to the movable coil (6). When the energy transmitted is-an equal magnetic field

15 の値よ 少 く るるため、 可動コィル (6)に作用する駆動力が低下 し該コィル (6)の運動モー ドに歪を生ずることにるるわけである。 これは可勣コィル (6)と交叉する磁力緩 (4)の平均磁束审度を 〔B〕 、 可動コ ィ ルの巻き全長を〔 〕 、 信号電流の大きさを 〔し〕 と した場 合の斥力〔F〕は :Since it is smaller than the value of 15, the driving force acting on the movable coil (6) is reduced, and the motion mode of the coil (6) is distorted. This is when the average magnetic flux intensity of the magnetic force ( 4 ) crossing the movable coil ( 6 ) is [B], the total winding length of the movable coil is [], and the magnitude of the signal current is [S]. The repulsive force [F] is:

20 F = k B . . . と 、 従って第 2図のよ うに可動コ イ ル (6)の進行方向に於いて 了 両後に交叉す可き磁力鎳 (4)の密妾が空隙 (3)内に於ける磁力線 (4)の20 F = k B... And, as shown in Fig. 2, the magnetic force 妾 crossing the movable coil (6) in the direction of travel is Of magnetic lines of force within (4)

. 教を第 1 図の平等磁界の場合の磁.力線 (4)の総数と等し と した 場合、 当然その歪のるい場合の平均〈直よ 低ぐ っていると考えIf the teaching is equal to the total number of field lines (4) in the case of the equal magnetic field shown in Fig. 1, naturally, the average in the case of low distortion is considered to be very low.

25 られる故可動コ イ ル (6)の駆動力は低下し歪が生ずるであろう と仮 定することで説明出来る。 更に信号電流が大と る程磁力線 (4)の 歪が大とるる故振巾歪が増大すると共に、 信号電流の変化に対し て駆動力の変化に位相遅れをも起す可能性がある。 As a result, it is assumed that the driving force of the movable coil (6) will decrease and distortion will occur. Can be explained. Furthermore, as the signal current increases, the distortion of the magnetic field lines (4) increases, so that the amplitude distortion increases, and a change in the signal current may cause a phase lag in the change in the driving force.

以上の悪影響を改善するため従来の技術と して、 空隙の磁界を 磁極表面附近で飽和に近つ'けて交叉磁界の影響を少¾ くする方法、 磁極の表面に導電性の短絡リ ングを篏めそれに可動コィルに流れ - る信号電流の 2次電流を流し、 その電流の発生する磁界によ J9交 叉磁界を打消す等の対策が取られている。 しかしながら磁極面の 磁界を飽和値まで近づけるには材料面での問題もあ 、 価格高に なる傾向をまぬかれず、 短絡リ ン グによる対策は可成 の効杲を 示すが低音甩スピ -力に於ける極低周波域での効果が低下する等 の欠点がある。  As a conventional technique to reduce the above adverse effects, a method of reducing the influence of the cross-magnetic field by reducing the influence of the cross magnetic field by approaching the magnetic field of the air gap near the magnetic pole surface to saturation, and a conductive short-circuit ring on the magnetic pole surface The secondary current of the signal current flowing through the movable coil is applied to it, and countermeasures such as canceling the J9 cross magnetic field by the magnetic field generated by the current are taken. However, there is a problem with the material in order to bring the magnetic field on the pole surface close to the saturation value, and there is a problem in terms of material, and the tendency to increase the price is not avoided, and the countermeasure by the short-circuit ring shows an effective effect. However, there is a drawback that the effect in the extremely low frequency range is reduced.

本発明は第 3 図に示す如く可動コィル (6)によ D発生する交叉磁 界 (8)を積極的に打消すために空隙 (3)内に補償コィル (11 )を設け、 該コ イ ル (11)に交叉磁界 (8)を打消すための電流を流すよ うにした もので、 使用材料の極端 ¾増加 ¾ しにその特性を改善することが 出来るものでるる。 補償コ イ ル (11 )に流す電流は可勣コィル (6)に 供耠される信号電流の莰形を別の増巾器で増巾するとか、 該信号 電流を変成器を通じるとかして得る方法も考えられるが、 最も簡 単る方法と しては可勣コィル (6)と補償コ イ ル (11 )を極性を考慮の 上直列に接続しその両端をそのスピー力の入力端子として取扱え ば良 のである。 改善される獰性と して、 音響出力の見掛け上の 歪の改善もさることるがら出力波形の位相特性、 特に低周波域で の ¾形の立上 特性に著しい改善が認められる。  In the present invention, as shown in FIG. 3, a compensating coil (11) is provided in an air gap (3) to positively cancel a cross magnetic field (8) generated by a movable coil (6). A current for canceling the cross magnetic field (8) is passed through the metal (11), and the characteristics can be improved with an extreme increase in the material used. The current flowing through the compensation coil (11) is obtained by amplifying the shape of the signal current supplied to the movable coil (6) by another amplifier or by passing the signal current through a transformer. Although the simplest method is conceivable, the simplest method is to connect a movable coil (6) and a compensation coil (11) in series considering the polarity and treat both ends as input terminals for the speed. It is good. As the fertility to be improved, not only the apparent distortion of the sound output is improved, but also the phase characteristics of the output waveform, particularly the rising characteristics of the ¾ shape in the low frequency range are remarkably improved.

次に第 4図はリ ボン又はリ ー フ状導体を使用したス ピーカの原 理を示す 1 例である。 対向する磁極(12),(13 ) によ 形成された 空隙(14)には磁力線 C15)によ ])ほ 平等 磁界が存在し、 空隙 (14)内に磁力線(15)と直交する方向にその全体に可撓性を持たせ るか、 或いは両端にのみ可撓性を持たせる ど矢印(16)の方向に _ 5可動 ¾様にして両端部を支持された可動導体(17)が位置する。 信 号電流が可動導体(17)に流れると磁力線 (15)との間に生ずる斥力 で可動導体(17)に矢印 〔16)の方向に駆動力が生じ運動するが、 同 時に可動導体(17)の周囲に生じた交叉磁界(18)のため第 5 図に示 すよ うに原磁界が乱される。 この結果前記コィル状導体を有するNext, Fig. 4 shows the source of a speaker using a ribbon or leaf-shaped conductor. This is an example showing the principle. The gap (14) formed by the opposing magnetic poles (12) and (13) has a magnetic field line C15). The movable conductor (17) supported at both ends by moving it in the direction of arrow (16) so that it has flexibility as a whole or only at both ends. I do. When a signal current flows through the movable conductor (17), a repulsive force generated between the movable conductor (17) and the magnetic field line (15) generates a driving force in the direction of the arrow [16] on the movable conductor ( 17 ) and moves. The original magnetic field is disturbed as shown in Fig. 5 due to the cross magnetic field (18) generated around (). This results in having the coiled conductor

10場合で説明したと同様 ¾理論によ D可動導体 (17)よ 直接、 或い はそれに接読されたサゥン ドラジェ— タ ょ 輻射される音響出力 に歪を生ずる。 か る磁界の歪を打消すため第 6 図に示すよ う可 動導体(17 )に接 して並行に固定して置かれた補償導体(19)に、 可動導体(17)に信号電流が流れて生ずる交叉磁界 (18)を打消すたSimilar to the case described in 10) (1) According to the theory, the sound output radiated directly from the sound conductor (17) or read out to the movable conductor (17) causes distortion. As shown in Fig. 6, the signal current is applied to the compensating conductor (19) fixed in parallel with the movable conductor (17) and the movable conductor (17) to cancel the distortion of the magnetic field. Crossed magnetic field (18) generated by flowing

15 めの電流を流すことによ その特性を改善出来るのである。 The characteristics can be improved by passing the other current.

頭記に述べた如く説明例をオーディ ォ用ス ピーカにとったが、 その他計測機器、 制御機器等の駆動部分に応用出来ることは勿論、 類似構造を有するマイクホ ン、 振動ピッ クアツ ブ等の電磁的発電 力を利用した機器に於 ても、 その発電コ イ ル、 発電リ ボン等に As described above, the explanation example was taken for audio speakers.However, it can be applied to other driving parts such as measurement equipment and control equipment, as well as electromagnetic equipment such as microphones and vibration pickups that have similar structures. Equipment that uses static power, such as power generation coils and power generation ribbons

20 流れる電流によ ])生ずる交叉磁界によ 原磁界が乱れその電気出 力波形に歪を生ずるが、 前記スピ—力の例と同様磁界内に補償コ ィル又は補償導体を設けそれに交叉磁界を打消すための電^を流 すことによ 出力の歪を改菩することが出釆るものである。 20 ) Due to the crossing magnetic field generated), the original magnetic field is disturbed and the electric output waveform is distorted. It is evident that the distortion of the output can be improved by passing electricity to cancel the magnetic field.

また第 3 図および第 6 図に示したよ うに空隙 (3),(14)の中に夫々 補償コィル (6)並びに^償導体(19)を設けた場合、 必然的に空隙 (3),  As shown in Fig. 3 and Fig. 6, when the compensation coil (6) and the compensation conductor (19) are provided in the gaps (3) and (14), the gaps (3) and

ΟΜΡΙ ΟΜΡΙ

1 · \νι?ο : (14)の寸法が増大するため総磁力線数が減少し能率低下等性能上 の不利を招く場合がある。 そのよ う ¾場合可動コィル (6)を使用し たものに就いては第 7 図に示すよ う中心磁極 (1)および外周磁極 (2) の両方又は何れか一方の空隙 (3)に接する面にその面に沿つて鑄 (20),(21) を設け、 その中に補償コ イ ル (11)を埋設し、 またリ ボ ン状或いはリ -フ状の可動導体(17)を使用したものに就いては第 8図に示すよ う対向する磁極(12),(13) の空隙(14)に接する面に 可勣導体(17)に沿って溝(22),(23) を設け、 その中に補償導体 (19)を埋納する。 かくすることによ 夫々の空隙 (3), (14) の実効 寸法の増加を少くすることが出来、 能率の低下を防ぐことが出来 るのである。 1 · \ νι? Ο: Since the dimension of (14) increases, the total number of lines of magnetic force decreases, which may lead to a disadvantage in performance such as a decrease in efficiency. In such a case, the one using the movable coil (6) is in contact with the air gap (3) of the center magnetic pole (1) and / or the outer magnetic pole (2) as shown in Fig. 7. Casting (20), (21) is provided along the surface, and a compensation coil (11) is buried in it, and a ribbon-shaped or leaf-shaped movable conductor (17) is used. As shown in Fig. 8, grooves (22) and (23) are formed along the conductor (17) on the surface of the opposing magnetic poles (12) and (13) in contact with the air gap (14). And the compensation conductor (19) is embedded in it. By doing so, it is possible to reduce the increase in the effective dimension of each of the gaps (3) and (14), and to prevent a decrease in efficiency.

発明を'実施するための最良の形態  BEST MODE FOR CARRYING OUT THE INVENTION

(1) コィル状導体を使用した場合 (1) When coiled conductor is used

第 9 図は本発明を実施したダイ ナ ミ ッ ク型ラ ウ ドスピー力の縦 断面図であ D、 空隙(24)内に中心磁極(25) よび外周磁極(26)の 表面に沿って補償コィル (27),〔28) を固定してある以外は一般的 なラウ ドスピー力と同様である。 補償コ イ ル (27), (28) は可動コ ィル (29)とほ 同じ巻線密度、 つま 可動コ イ ル (29)の軸心方向 の単位長さに於ける巻数とほ 同じ卷数、 図のよ うに補償コ イ ル 'を 2つに分けた場合はその合計数と しその長さは大略可勣コ ィル (29)と同じ長さ いしは空隙 (24)に於ける磁界の有効長と同 じ位の長さの範囲とする。 その接読はたとえば第 10図に示すよ う に可動コ イ ル (29)と補償コィル (27),〔28) を共通の電流が流れた 時夫々 のコィルが発生する交叉磁界の向きが互に逆にるる様直列 に される。  FIG. 9 is a vertical cross-sectional view of a dynamic loud-speech force embodying the present invention D, which is compensated for in the air gap (24) along the surfaces of the center pole (25) and the outer pole (26). This is the same as general loud-speaking force except that coils (27) and [28] are fixed. The compensation coils (27) and (28) have the same winding density as the movable coil (29), that is, the same number of turns as the unit length in the axial direction of the movable coil (29). If the compensation coil 'is divided into two as shown in the figure, the total number will be the total number, and the length will be roughly the same as the length of the movable coil (29) or in the gap (24) The range is the same length as the effective length of the magnetic field. For example, as shown in Fig. 10, the direction of the crossing magnetic field generated by each coil when a common current flows through the movable coil (29) and the compensation coil (27), [28] is read as shown in Fig. 10. It is connected in series so that it is reversed.

Ο ΡΙΟ ΡΙ

V IPO (2) リ ボン状或 はリ ーフ状導体を使用した場合 V IPO (2) When using a ribbon-shaped or leaf-shaped conductor

第 11図は本発明を実施したス ー力の · 2面図であ Ϊ)、 磁極(3Q) , (31)によ ] 形成された空隙 (32)内に可動導体(33 )に平行してそれ を挾んだ形で補償導体(34)を設けた以外は従来のスピ -力 と同様 である。 補償導体(34)はその中を可動導体 (33 )の中を流れた信号 電流が折返して逆向きに流れるよ う、 つま ]?補償導体 (34)と可動 導体の発生する交叉磁界が互に逆向きにるる よ う接続される。  FIG. 11 is a two-sided view of the soot force implementing the present invention. FIG. 11) shows the magnetic poles (3Q) and (31)] formed in the gap (32) formed parallel to the movable conductor (33). This is the same as the conventional spin force except that the compensating conductor (34) is provided so as to sandwich it. The compensating conductor (34) and the crossing magnetic field generated by the movable conductor are arranged so that the signal current flowing in the movable conductor (33) turns back and flows in the opposite direction. Connected so that it is upside down.

(3) 能率を低下させない実施法  (3) Implementation method that does not reduce efficiency

補償コ ィ ノレ又は補償導体を設けるための空隙寸法増大による能 率低下を防ぐため、 コ イ ル状導体を使用したものについては第 12 図に示すよ うに磁極(25 ),(26 ) の空隙 〔24)に接する面に可動コィ ル (29 )の巻方向に沿つて溝 (35 ) , ( 36 ) を設け、 その中に補償コィ ル (27 ),(28 ) を埋納する。 かくすることによ 空隙(24)の寸法増 大を少く済ませることが出来、 能率低下を防ぐこ とが出来る。  As shown in Fig. 12, the gaps between the magnetic poles (25) and (26) are shown in Fig. 12 in order to prevent a decrease in efficiency due to an increase in the gap size for providing a compensation coil or compensation conductor. Grooves (35) and (36) are provided on the surface in contact with [24] along the winding direction of the movable coil (29), and compensation coils (27) and (28) are embedded in them. By doing so, the increase in the size of the gap (24) can be reduced, and a decrease in efficiency can be prevented.

同様リ ボン又は リ ーフ状導体を使用したものにあつては第 13図 に示すよ うに磁極(30 ) , (31 ) の空隙(32)に接する面に可動導体 (33)に沿って溝(37)を設け、 その中に補償導体(34)を埋納する。  Similarly, in the case of using a ribbon or leaf-shaped conductor, as shown in Fig. 13, a groove is formed along the movable conductor (33) on the surface of the magnetic poles (30), (31) in contact with the gap (32). (37) is provided, and the compensating conductor (34) is embedded in it.

図面の簡単 る説明  BRIEF DESCRIPTION OF THE DRAWINGS

第 1 図よ ]9第 8図までは「発明の開示」 に対する説明用、 第 9 図よ !)第 12図までは「発明を実施するための最良の形態」 に対す る説明用の図面である。  Fig. 1] 9 Up to Fig. 8 is for explanation of "Disclosure of invention", Fig. 9! ) Figures up to Fig. 12 are drawings for explaining "the best mode for carrying out the invention".

第 1 図はコィ ル状導体を使用したラ ゥ ドス ビーカにおいて交叉 磁界の発生を示す図面、 苐 2 図は交叉磁界によ ]5磁力線の乱れた 状態を示す図面、 第 3 図は交叉磁界を打消すための補價コィ ルを 設けた図面である。 第 4図はリ ボン又はリ一フ状導体を使用したスピー力に於 て 交叉磁界の発生を示す図面、 第 5 図は交叉磁界によ 磁力線の乱. れた状態を示す図面、 第 6 図は交叉磁界を打消すための補償導体 を設けた図面である。 Fig. 1 is a drawing showing the generation of a crossing magnetic field in a radiating beaker using a coil-shaped conductor. It is a drawing provided with a compensation coil for canceling. Fig. 4 is a drawing showing the generation of a crossover magnetic field by the speed using a ribbon or a leaf-shaped conductor. Fig. 5 is a drawing showing the state where the magnetic field lines are disturbed by the crossing magnetic field. Is a drawing provided with a compensating conductor for canceling the cross magnetic field.

第 7 図は補償コ イ ルを、 第 8 図は補償導体を夫々磁極面に設け た溝の中に埋鈉した例を示す図面で ¾る。  FIG. 7 is a drawing showing an example in which a compensation coil is embedded, and FIG. 8 is a drawing showing an example in which a compensation conductor is embedded in a groove provided on each magnetic pole surface.

第 9 図、 第 10図はコィル状導体を使用したラ ウ ドス ビー力に本 発明を実施した例を示す図面である。  FIG. 9 and FIG. 10 are drawings showing an example in which the present invention is applied to a Loudsby force using a coil-shaped conductor.

第 11図は リ ボン状又はリ ーフ状導体を使用したス ピーカに本発 明を実施した例を示す図面である。  FIG. 11 is a diagram showing an example in which the present invention is applied to a speaker using a ribbon-shaped or leaf-shaped conductor.

第 12図は補償コ ィ ルを、 第 13図は補償導体を夫々磁極の表面に 設けた溝に埕納した例を示す図面である。  FIG. 12 is a drawing showing an example in which the compensation coil is stored, and FIG. 13 is an example in which the compensation conductor is stored in grooves provided on the surface of the magnetic pole.

ΟΙ.ίΡΙ ΟΙ.ίΡΙ

Claims

図面の引用符号の説明 Description of reference numerals in drawings (1) 「発明の開示」用図面中夫々 - (1) Each of the drawings for "Disclosure of Invention"- 1 …中心磁極、 2 …外周 ¾極、 3 …空隙、 4 …磁力線、 5 … ボビン、 6 …可動コ イ ル、 7 … ( 可動コ イ ルの運動方 向を示す) 矢印、 8 …交叉磁界、 9 … (交叉磁界の向きを 示す) 矢印、 10… ( 可動コィ ルに駆動力の作用した向きを示 す ) 矢印、 11…補償コ イ ル、 12…磁極、 13…磁極、 1… Center magnetic pole, 2… Outer circumference ¾pole, 3… Gap, 4… Line of magnetic force, 5… Bobbin, 6… Movable coil, 7… (Indicates the direction of movement of the movable coil) , 9… (indicates the direction of the cross magnetic field), 10… (indicates the direction in which the driving force acts on the movable coil), 11, 11… compensation coil, 12… magnetic pole, 13… magnetic pole, 14…空隙、 15…磁力線、 16— (可動導体の違動する方向を 示す) 矢印、 17…可動導体、 18…交叉磁界、 19…補償導 体、 20 ( 中心磁極に設けた ) 溝、 21… ( 外周磁極に設け た )溝、 22— (磁極((12))に設けた )溝、 23.… (磁極((13)) に設けた )溝 - である 0  14 ... air gap, 15 ... magnetic field lines, 16-(indicating the direction in which the movable conductor moves) arrow, 17 ... movable conductor, 18 ... cross magnetic field, 19 ... compensating conductor, 20 (provided in the center magnetic pole) groove, 21 … Groove (provided on the outer magnetic pole), 22—groove (provided on the magnetic pole ((12))), 23.… groove (provided on the magnetic pole ((13))) 0 (2) 「発明を実施するための最良の形態」用図面中夫々  (2) Each of the drawings for "Best mode for carrying out the invention" 24…空隙、 25…中心磁極、 26…外周磁極、 27…補償コィ ル、 28…補償コ イ ル、 29 -•可動コィル、 30…磁極、  24 ... air gap, 25 ... center magnetic pole, 26 ... outer peripheral magnetic pole, 27 ... compensation coil, 28 ... compensation coil, 29-movable coil, 30 ... magnetic pole, 31…磁極、 32…空隙、 33 ·- -可勣導体、 34…補償導体、 35… ( 中心磁極に設けた )溝、 36… ( 外周磁極に設けた ) 壽、 37 (磁極に設けた ) 濤  31 ... magnetic pole, 32 ... air gap, 33 ·--movable conductor, 34 ... compensation conductor, 35 ... groove (provided on the center magnetic pole), 36 ... (provided on the outer magnetic pole), 37 (provided on the magnetic pole) Toto である。 10 It is. Ten 請 求 の 範 囲  The scope of the claims 磁極の空隙に接す'る面よ 可勣コィ ル又は可動導体に至る間或 は磁極の表面に設けた壽内に置かれた補償コ ィル又は補 ί«導体 に可勣コィル又は可動導体に信号電流が流れて発生する交叉磁界 を打消すための電流を流すことを特徵とする電磁的駆動および発 A compensation coil or movable conductor placed between the movable coil and the movable conductor or within the life span provided on the surface of the magnetic pole from the surface in contact with the gap of the magnetic pole. Electromagnetic drive and generator characterized by flowing a current to cancel the cross magnetic field generated by the signal current flowing through ¾ ^ 0 ¾ ^ 0 O PI O PI 、、 ATI0  ,, ATI0
PCT/JP1981/000035 1980-02-26 1981-02-21 Magnetic circuit for an electro-mechanical transducer of a dynamic electricity-type Ceased WO1981002501A1 (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
JP2389980A JPS57131200A (en) 1980-02-26 1980-02-26 Electromagnetic driving system
JP80/23899 1980-02-26

Publications (1)

Publication Number Publication Date
WO1981002501A1 true WO1981002501A1 (en) 1981-09-03

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ID=12123303

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Country Link
JP (1) JPS57131200A (en)
WO (1) WO1981002501A1 (en)

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0116957A1 (en) * 1983-02-22 1984-08-29 Apogee Acoustics, Inc. Ribbon speaker system
EP0350652A1 (en) * 1988-07-15 1990-01-17 Studer Revox Ag Electrodynamic loudspeaker
WO1991005447A1 (en) * 1989-10-02 1991-04-18 Jbl, Incorporated Improved electrodynamic loudspeaker
US5062140A (en) * 1988-04-27 1991-10-29 Sony Corporation Induction speaker
US5832096A (en) * 1993-01-06 1998-11-03 Velodyne Acoustics, Inc. Speaker containing dual coil
WO2002093976A1 (en) * 2001-05-17 2002-11-21 Twin Saver Co., Ltd. Sound-to-vibration conversion apparatus
US6768806B1 (en) 1998-03-19 2004-07-27 Harman International Industries, Incorporated Shorting rings in dual-coil dual-gap loudspeaker drivers
US20230111935A1 (en) * 2020-03-25 2023-04-13 Lorentz Audio B.V. Electroacoustic transducer and loudspeaker, microphone and electronic device comprising said electroacoustic transducer

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2016539562A (en) * 2013-11-06 2016-12-15 ダンマルクス テクニスケ ウニベルシテット Loudspeaker assembly with flux modulation distortion suppression

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS504241B1 (en) * 1969-12-08 1975-02-17
JPS51161812U (en) * 1975-06-17 1976-12-23
JPS51151122A (en) * 1975-06-19 1976-12-25 Sansui Electric Co Speaker unit
JPS5482228A (en) * 1977-12-14 1979-06-30 Matsushita Electric Ind Co Ltd Converter

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS504241B1 (en) * 1969-12-08 1975-02-17
JPS51161812U (en) * 1975-06-17 1976-12-23
JPS51151122A (en) * 1975-06-19 1976-12-25 Sansui Electric Co Speaker unit
JPS5482228A (en) * 1977-12-14 1979-06-30 Matsushita Electric Ind Co Ltd Converter

Cited By (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0116957A1 (en) * 1983-02-22 1984-08-29 Apogee Acoustics, Inc. Ribbon speaker system
US4550228A (en) * 1983-02-22 1985-10-29 Apogee Acoustics, Inc. Ribbon speaker system
US5062140A (en) * 1988-04-27 1991-10-29 Sony Corporation Induction speaker
EP0350652A1 (en) * 1988-07-15 1990-01-17 Studer Revox Ag Electrodynamic loudspeaker
US5129005A (en) * 1988-07-15 1992-07-07 Studer Revox Ag Electrodynamic loudspeaker
WO1991005447A1 (en) * 1989-10-02 1991-04-18 Jbl, Incorporated Improved electrodynamic loudspeaker
US5832096A (en) * 1993-01-06 1998-11-03 Velodyne Acoustics, Inc. Speaker containing dual coil
US6768806B1 (en) 1998-03-19 2004-07-27 Harman International Industries, Incorporated Shorting rings in dual-coil dual-gap loudspeaker drivers
WO2002093976A1 (en) * 2001-05-17 2002-11-21 Twin Saver Co., Ltd. Sound-to-vibration conversion apparatus
US20230111935A1 (en) * 2020-03-25 2023-04-13 Lorentz Audio B.V. Electroacoustic transducer and loudspeaker, microphone and electronic device comprising said electroacoustic transducer

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