WO2013076914A1 - スピーカおよびスピーカを備えた電子機器 - Google Patents
スピーカおよびスピーカを備えた電子機器 Download PDFInfo
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- WO2013076914A1 WO2013076914A1 PCT/JP2012/006766 JP2012006766W WO2013076914A1 WO 2013076914 A1 WO2013076914 A1 WO 2013076914A1 JP 2012006766 W JP2012006766 W JP 2012006766W WO 2013076914 A1 WO2013076914 A1 WO 2013076914A1
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- diaphragm
- voice coil
- speaker
- speaker according
- coil bobbin
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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
- H04R9/025—Magnetic circuit
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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
- H04R7/00—Diaphragms for electromechanical transducers; Cones
- H04R7/02—Diaphragms for electromechanical transducers; Cones characterised by the construction
- H04R7/12—Non-planar diaphragms or cones
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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
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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
- H04R2209/00—Details of transducers of the moving-coil, moving-strip, or moving-wire type covered by H04R9/00 but not provided for in any of its subgroups
- H04R2209/022—Aspects regarding the stray flux internal or external to the magnetic circuit, e.g. shielding, shape of magnetic circuit, flux compensation coils
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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
- H04R2209/00—Details of transducers of the moving-coil, moving-strip, or moving-wire type covered by H04R9/00 but not provided for in any of its subgroups
- H04R2209/041—Voice coil arrangements comprising more than one voice coil unit on the same bobbin
Definitions
- the present disclosure relates to a speaker, and more specifically, to a speaker that is thinned.
- a speaker unit for a television (hereinafter referred to as a speaker) is usually attached on both sides of a display such as a plasma display or a liquid crystal display, which contributes to an increase in the width of the television set. For this reason, a speaker having an elongated structure such as a rectangular shape or an elliptical shape has been conventionally used for television. In addition, as the display display becomes longer, it is required to further reduce the width of the speaker. In addition, since thin TVs using plasma displays and liquid crystal displays are increasing, there is a further demand for thinner speakers. Further, there is a demand for speakers to improve the sound quality of the sound corresponding to the high image quality of the screen.
- Patent Document 1 is known as a prior art document related to the present disclosure, and Patent Document 1 shows the structure of a conventional elongated speaker.
- the conventional elongated speaker employs a driving method of driving the central portion of the elongated diaphragm, split resonance tends to occur in the longitudinal direction of the diaphragm.
- the frequency characteristic related to the reproduction sound pressure level becomes a characteristic that causes a peak dip in the middle and high ranges, and the sound quality is deteriorated.
- the diaphragm in order to make it difficult to cause resonance in the longitudinal direction with the same opening area, it is necessary to make the diaphragm have a deep shape (cone shape), and there is a problem that the depth of the speaker cannot be reduced. .
- the present disclosure has been made in view of the above-described problems, and an object thereof is to provide a speaker that can be thinned and has excellent sound quality even though it has an elongated structure.
- a speaker with an elongated structure in which a frame and a planar shape perpendicular to the vibration direction have a long and short shape, and a hollow diaphragm and a diaphragm are supported so as to vibrate.
- An edge to be fixed at least one cylindrical voice coil bobbin connected through the diaphragm, a voice coil fixed to the voice coil bobbin inside the hollow structure of the diaphragm, and inside the voice coil bobbin And a magnetic circuit for driving the voice coil.
- FIG. 1A is a top view of the speaker according to Embodiment 1.
- FIG. 1B is a schematic cross-sectional view taken along line A-A ′ of FIG. 1A.
- FIG. 1C is a schematic cross-sectional view taken along B-B ′ of FIG. 1A.
- 2A is a top view of the diaphragm according to Embodiment 1.
- FIG. 2B is a schematic cross-sectional view taken along line E-E ′ of FIG. 2A.
- 2C is a schematic cross-sectional view taken along the line F-F ′ of FIG. 2A.
- FIG. 3 is a perspective view of the voice coil and the voice coil bobbin in the first embodiment.
- FIG. 4 is a perspective view of the magnetic circuit according to the first embodiment.
- FIG. 5 is a component configuration perspective view of the speaker in the first embodiment.
- FIG. 6A is a hollow semicircular cross-sectional model diagram.
- FIG. 6B is a cross-sectional model diagram of a hollow circle.
- FIG. 7 is a diagram showing calculated values of the second moment of section, the turning radius, and the sectional area when the sectional shape is a hollow circle and a hollow semicircle.
- FIG. 8 is a diagram illustrating the analysis result of the resonance frequency of the natural vibration mode of the diaphragm having a hollow circular shape and a hollow semicircular cross-sectional shape.
- FIG. 9A is a top view of the diaphragm according to the second exemplary embodiment.
- FIG. 9A is a top view of the diaphragm according to the second exemplary embodiment.
- FIG. 9B is a cross-sectional view in the longitudinal direction of the diaphragm according to the second exemplary embodiment.
- 10A is a top view of the speaker according to Embodiment 3.
- FIG. 10B is a schematic cross-sectional view taken along the line G-G ′ of FIG. 10A.
- FIG. 11A is a top view of the speaker according to Embodiment 3.
- FIG. 11B is a schematic cross-sectional view taken along the line H-H ′ of FIG. 11A.
- FIG. 12A is a characteristic diagram in the case of two-point drive for controlling the primary resonance mode.
- FIG. 12B is a characteristic diagram in the case of four-point drive for controlling both the primary and secondary resonance modes.
- FIG. 12C is a characteristic diagram in the case of center driving.
- FIG. 12A is a characteristic diagram in the case of two-point drive for controlling the primary resonance mode.
- FIG. 12B is a characteristic diagram in the case of four-point drive for controlling both the primary
- FIG. 13 is a perspective view of a magnetic circuit according to the fifth embodiment.
- FIG. 14 is a cross-sectional view of the speaker in the short direction in the fifth embodiment.
- FIG. 15 is a perspective view of a magnetic circuit according to the sixth embodiment.
- FIG. 16 is a cross-sectional view of the speaker according to Embodiment 6 in the short direction.
- FIG. 17 is a perspective view of the component configuration of the speaker in the sixth embodiment.
- FIG. 18 is a diagram of a mobile information terminal device.
- FIG. 19 is a diagram of an image display device.
- FIG. 20 is a mounting diagram of a vehicle-mounted speaker.
- FIG. 21A is a top view of a conventional speaker.
- FIG. 21B is a cross-sectional view in the I-I ′ direction of FIG. 21A.
- FIG. 21C is a cross-sectional view in the J-J ′ direction of FIG. 21A.
- FIG. 22 is a sound pressure frequency characteristic diagram of a
- FIG. 21A is a plan view of a conventional elongated speaker 1000.
- FIG. 21B is a schematic cross-sectional view taken in the longitudinal direction (I-I ′) of FIG. 21A and viewed from the arrow i.
- FIG. 21C is a schematic cross-sectional view taken in the short direction (J-J ′) and viewed from the arrow j.
- a conventional elongated speaker 1000 includes a magnet 1001, a plate 1002, a yoke 1003, a frame 1004, a voice coil bobbin 1005, a voice coil 1006, a damper 1007, a diaphragm 1008, A dust cap 1009 and an edge 1010 are provided.
- the arrangement of main components will be described below.
- the voice coil 1006 is a winding of a conductor such as copper or aluminum, and is fixed to one of the cylindrical voice coil bobbins 1005.
- the voice coil 1006 is arranged in a magnetic gap formed by the magnet 1001 between the plate 1002 and the yoke 1003.
- a diaphragm 1008 is fixed to the other side of the voice coil bobbin 1005.
- the voice coil bobbin 1005 is fixed by a damper 1007.
- the damper 1007 is connected to the frame 1004.
- the plate 1002 is inside the voice coil bobbin 1005 and is disposed at a place where the voice coil 1006 is fixed.
- a magnet 1001 is disposed below the plate 1002, and a yoke 1003 is disposed so as to partially surround the magnet 1001.
- the planar shape of the diaphragm 1008 is an ellipse or a substantially ellipse.
- the diaphragm 1008 has a so-called cone shape having an inclination toward the center.
- cone paper or the like is used as the material of the diaphragm 1008, cone paper or the like is used.
- a dust cap 1009 is fixed to the center of the diaphragm 1008.
- the edge 1010 has an annular planar shape and a semicircular cross section. Further, the inner peripheral portion of the edge 1010 is fixed to the outer peripheral portion of the diaphragm 1008, and the outer peripheral portion of the edge 1010 is fixed to the frame 1004.
- the operation of the conventional slender speaker 1000 configured as described above will be described.
- the voice coil bobbin 1005 moves in a vertical direction with the dust cap in the upward direction in FIG. 21B due to the current applied to the voice coil 1006 and the magnetic field around the voice coil 1006. I do.
- the diaphragm 1008 vibrates in the direction of the piston movement. As a result, sound waves are radiated from the diaphragm 1008.
- FIG. 22 is a diagram showing frequency characteristics related to the reproduction sound pressure level of the conventional elongated speaker 1000.
- the vertical axis represents the reproduction sound pressure level when 1 W of power is input to the conventional elongated speaker 1000
- the horizontal axis represents the drive frequency.
- the microphone for measuring the reproduction sound pressure level is arranged on the central axis of the conventional elongated speaker 1000 and at a position 1 m away from the conventional elongated speaker 1000 on the front side. To do.
- the conventional elongated speaker 1000 as described above has the following problems. Since the conventional elongated speaker 1000 employs a driving method of driving the central portion of the elongated diaphragm 1008, split resonance is likely to occur in the longitudinal direction. As a result, the frequency characteristic related to the reproduction sound pressure level is a characteristic that causes a peak dip in the middle and high ranges, and the sound quality is deteriorated. For example, in the characteristics shown in FIG. 22, noticeable dip is observed in the vicinity of 2 kHz, 3 kHz, and 5 kHz.
- the diaphragm 1008 has a deep shape (cone shape). That is, the diaphragm 1008 has a shape having a height in the vertical direction in FIG. 21B. Further, when the vibration plate 1008 vibrates, a distance is provided to prevent the damper 1007 and the frame 1004 from contacting the magnetic circuit such as the yoke 1003 and the plate 1002 and the damper 1007 and the vibration plate 1008.
- the damper 1007 is fixed near the center of the voice coil bobbin 1005.
- the diaphragm 1008, the upper part of the voice coil bobbin 1005, the damper 1007, the lower part of the voice coil bobbin 1005, the magnet 1001, the plate 1002, and the yoke 1003 are spaced apart in the vibration direction (vertical direction in FIG. 21B). It will be provided and arranged. With the above configuration, the depth of the speaker cannot be reduced.
- the present inventors have been able to obtain a flat frequency characteristic in which split resonance is difficult to occur while having a slender structure, suppress the occurrence of peak dip, and further achieve a thin speaker with excellent sound quality that realizes a reduction in thickness.
- Invented the structure Various aspects of the present disclosure based on this idea are as follows.
- a speaker includes a frame, a vertically long shape having a plane that is perpendicular to a vibration direction, and a diaphragm having a hollow structure, and a diaphragm that supports the diaphragm so that the diaphragm can vibrate.
- An at least one cylindrical voice coil bobbin connected through the diaphragm, a voice coil fixed to the voice coil bobbin within the hollow structure of the diaphragm, and an interior of the voice coil bobbin And a magnetic circuit for driving the voice coil.
- the components are not stacked in the thickness direction of the speaker, but are arranged so as to be nested inside each other in the hollow structure of the diaphragm, thereby realizing a reduction in thickness. can do.
- the voice coil is fixed so that the height of the voice coil bobbin is equally divided, and the center of gravity of the voice coil, the fixing point of the edge to the frame, and the center of gravity of the diaphragm And the center of gravity of the magnetic circuit are arranged on the same plane.
- the moment that the vibration system tends to rotate can be minimized and the rolling resistance can be improved.
- a grommet is caulked at the longitudinal end portion of the diaphragm, a conductive wire connecting the grommet and a terminal provided on the frame, and a lead wire connected from the grommet to the voice coil;
- the lead wire can be fixed inside the diaphragm.
- the speaker can be made thin.
- the magnetic circuit includes a configuration in which two magnets are fixed in a repulsive direction, or a cross-sectional shape in the short direction of the diaphragm is a circular shape, an oval shape, a hollow trapezoidal shape, or It can be a hollow polygon.
- two voice coil bobbins may be provided, and the voice coil bobbins may be arranged one by one at the nodes of the primary resonance mode in the longitudinal direction of the diaphragm.
- four voice coil bobbins may be provided, and the voice coil bobbins may be disposed at the nodes of the primary resonance mode and the secondary resonance mode in the longitudinal direction of the diaphragm.
- the driving point of the diaphragm is arranged at a position where the primary and secondary resonance modes are suppressed, and it is possible to realize an expansion of the reproduction frequency band.
- an auxiliary plate or an auxiliary magnet is used in the magnetic circuit of the speaker, the shape of both ends in the longitudinal direction of the diaphragm is a hemispherical shape, or the speaker is provided in an electronic device. It is also possible.
- FIG. 1A is a top view of the speaker 100 according to the present embodiment.
- 1B is a schematic cross-sectional view taken along the line AA ′ in FIG. 1A and viewed from the direction of arrow a.
- 1C is a schematic cross-sectional view taken along the line BB ′ in FIG. 1A and viewed from the direction of the arrow b.
- the speaker 100 includes a diaphragm 110, a voice coil 120, a voice coil bobbin 130, a magnetic circuit 140, an edge 150, a frame 160, and a dust cap 170. As shown in FIG. 1A, the speaker 100 has an elongated shape with different lengths in the vertical direction and the horizontal direction. Hereinafter, each configuration of the speaker 100 will be described.
- FIG. 2A is a plan view of the diaphragm 110, and shows only the left side from the line C-C 'in
- FIG. 2B is a schematic cross-sectional view taken along the line E-E ′ in FIG. 2A and viewed from the direction of the arrow e.
- 2C is a schematic cross-sectional view taken along the line F-F ′ in FIG. 2A and viewed from the direction of the arrow f.
- the planar shape of diaphragm 110 viewed from the vibration direction (direction perpendicular to the paper surface in FIG. 2A) has a long side and a short side.
- the both ends of the longitudinal direction of the diaphragm 110 have a hollow hemispherical structure.
- the cross-sectional shape of the diaphragm 110 in the short direction is a hollow circular shape.
- the diaphragm 110 includes an upper diaphragm 111a and a lower diaphragm 111b each having an elongate track provided with a bonding portion 112 at a terminal portion having a semicircular cross section in the short direction. Are pasted together.
- the diaphragm 110 has the cross-sectional shape as described above, the diaphragm 111a and the diaphragm 111b having an elongated track may not be bonded as described above. Further, as shown in FIG. 1A, the diaphragm 110 is provided with a through hole 180 for fixing the voice coil bobbin 130. In the case where the diaphragm 111a and the diaphragm 111b are bonded together as in this embodiment, the diaphragm 111a and the diaphragm 111b are provided with through holes 180, respectively.
- the material of the diaphragm 110 a material that is suitable for thinning and lightweight is desirable, and it is most preferable to use paper or a polymer film.
- a light and highly rigid metal foil such as aluminum or titanium may be used.
- FIG. 3 is a perspective view of the voice coil 120 and the voice coil bobbin 130.
- the voice coil 120 is formed by winding a thin wire made of copper or aluminum, which is insulated, on a side surface of a cylindrical voice coil bobbin 130 having an oval cross section. Further, the voice coil 120 is disposed at an intermediate point on the side surface of the voice coil bobbin 130. That is, the distance ⁇ from the line that bisects the height of the voice coil 120 shown in FIG. 3 to the upper end of the voice coil bobbin 130 and the lower end of the voice coil bobbin 130 from the line that bisects the height of the voice coil 120.
- the voice coil 120 is wound and fixed on the side surface of the voice coil bobbin 130 so that the distance ⁇ to the portion becomes equal.
- FIG. 4 is a perspective view of the magnetic circuit 140.
- the size of the magnetic circuit 140 is smaller than the inner diameter of the voice coil bobbin 130 so as to be disposed inside the voice coil bobbin 130, and the outer diameter shape of the magnetic circuit 140 is similar to the voice coil bobbin 130.
- the magnetic circuit 140 has two magnetized magnets 141 fixed in directions that repel each other, and in each magnet 141, a plate 142 is provided on the surface opposite to the surface on which the magnet 141 is fixed. It is fixed.
- the letters N and S are shown in FIG. The polarities of N and S are repulsive polarities and have a reversible relationship.
- the generated magnetic flux exits from the joint surface 143 of the two magnets 141 in the horizontal direction and then reaches the plate 142 while repelling each other. Further, the magnetic circuit 140 is fixed to the frame 160 by fixing the end surface of one plate 142 to the frame 160.
- the edge 150 will be described.
- the planar shape of the edge 150 is annular.
- the edge 150 has a substantially semicircular or semi-elliptical cross section perpendicular to the vibration direction (the vertical direction with the dust cap 170 in the upward direction in FIGS. 1B and 1C). is there.
- the outer periphery of the diaphragm 110 is fixed to the inner periphery of the edge 150.
- the frame 160 As shown in FIGS. 1A to 1C, the frame 160 has an annular shape having an opening. As shown in FIGS. 1A to 1C, the outer periphery of the edge 150 is fixed to the opening of the frame 160.
- the dust cap 170 As shown in FIGS. 1B and C, the dust cap 170 is provided at the upper end of the voice coil bobbin 130. The dust cap 170 passes through the through hole 180 and blocks sound emitted from the upper surface of the voice coil bobbin 130 in the vibration direction.
- FIG. 5 is a component configuration perspective view of the speaker 100 of the present embodiment.
- the voice coil bobbin 130 is inserted into the through hole 180 of the diaphragm 110. Further, the fixed point of the edge 150 on the frame 160, the center of gravity of the diaphragm 110, the center of gravity of the voice coil 120, and the center of gravity of the magnetic circuit 140 are disposed on the same plane. In the case of the present embodiment, it is disposed inside the annular cross section of the diaphragm 110 and on the center plane (X-X ′ plane in FIG. 1B) of the diaphragm 110 orthogonal to the vibration direction.
- the outer periphery of the diaphragm 110 is normally supported by the edge 150, it can be regarded as a rod that is free at both ends. Therefore, from the theory of the vibration mode of the free rod at both ends, it is possible to consider changes due to the resonance frequency of the vibration mode and the cross-sectional shape of the rigidity. Here, the theory of the vibration mode of the free rod at both ends will be described.
- the following equation (1) shows the resonance frequency equation of the vibration mode of the rod with free ends.
- l is the length of the rod
- ⁇ is the density
- Q is the Young's modulus of the material
- K is the radius of rotation.
- FIG. 6A shows a hollow semicircular cross-sectional shape of diaphragm 610
- FIG. 6B shows a hollow circular cross-sectional shape of diaphragm 110 of the present embodiment.
- FIG. 6A and 6B will be used to explain the radius of rotation for each cross-sectional shape.
- the hollow semicircular cross-sectional shape of FIG. 6A will be described.
- the secondary moment of the figure of a hollow section such as a pipe or tunnel is obtained by subtracting the secondary moment of the figure of the hollow figure from the secondary moment of the figure of the outer figure. Can do.
- the position of the centroid of the outer graphic is different from the position of the centroid of the inner graphic with respect to the reference axis for obtaining the cross-sectional moment, but in the case of a hollow semicircular cross-sectional shape such as the diaphragm 610 Since the thickness of the diaphragm 610 is very thin, the radius of the outer semicircle and the inner semicircle may be considered to be substantially equal. Therefore, the cross-sectional secondary moment of the hollow semicircle is considered as a difference between the cross-sectional secondary moments of the outer and inner semicircles.
- the following formula (2) shows the non-hollow semicircular cross-sectional moment of moment
- the following formula (3) shows the cross-sectional secondary moment of hollow semicircular shape
- the following formula (4) shows: The cross-sectional area is shown.
- r semi indicates a radius of a semicircle that is not hollow.
- R represents the radius of the outer semicircle
- r represents the radius of the inner semicircle
- the turning radius is the square root of the quotient obtained by dividing the sectional moment of inertia by the sectional area
- the turning radius of the hollow semicircular sectional shape is expressed by the following formula (5).
- R represents the radius of the outer semicircle
- r represents the radius of the inner semicircle
- FIG. 7 shows the secondary moments of the cross section, the radius of rotation, and the cross sectional area of each of the hollow circular shape and hollow semicircular cross sectional shape calculated using the above equations (3) to (8).
- the turning radius is about 1.9 times from the above formulas (5) and (7), and the above formulas (2) and ( 6) shows that the moment of inertia of the cross section is about 7.2 times, so that the resonance frequency is about 1.9 times higher and the rigidity is improved about 7.2 times.
- the resonance frequency of the natural vibration mode by the finite element method (Finite Element Method (FEM)) incorporating the actual shape model of the diaphragm 110 and the diaphragm 610 described in the present embodiment.
- FEM Finite Element Method
- the resonance mode is evaluated only when the number of nodes is an even number.
- a resonance with two nodes is represented as a primary mode, and a case with four nodes is represented as a secondary mode. This is because when the resonance mode contributing to the sound pressure is an odd number of nodes, the disturbance of the sound pressure due to the resonance mode is canceled on the axis and a peak dip occurs only when the number of nodes is an even number. Because there is.
- FIG. 8 shows that the theoretical calculation value (theoretical value) and the simulation analysis value (FEM value) are in good agreement. Further, it can be seen that the resonance frequency of the diaphragm 110 having a circular cross section is about twice as high as that of the diaphragm 610 having a semicircular cross section. From the frequency change of the simulation result, the change in rigidity due to the change in the cross-sectional shape of the diaphragm from the semicircular shape to the circular shape is calculated backward.
- the resonance frequency is proportional to the radius of rotation.
- the turning radius is the square root of the quotient of the sectional moment of inertia and the sectional area
- the sectional moment of inertia is proportional to the product of the square of the turning radius and the sectional area. Therefore, it can be seen from FIG. 8 that when the cross-sectional shape of the diaphragm is changed from a semicircular shape to a circular shape, the change in the radius of rotation is about twice and the cross-sectional area is also doubled, so that the rigidity is about eight times. .
- the rigidity in the longitudinal direction of the diaphragm can be improved and the resonance frequency of the mode can be increased.
- the number of resonance frequencies that have an influence on an important voice band can be reduced.
- the cross section in the short direction of diaphragm 110 has been described as a circular diaphragm.
- the rigidity of the diaphragm 110 can be further improved by making the cross section in the short direction of diaphragm 110 into an oval shape. Can be high.
- the cross-sectional shape of the diaphragm 110 in the short direction may be a hollow trapezoid or a hollow polygon.
- the vibration plate 110 has a hollow circular cross section and increases the second moment of the cross section, thereby increasing the rigidity.
- the radius of the cylinder is 2.0 mm
- the overall height of the diaphragm 110 is about 4.0 mm.
- the total height is about 20 to 30 mm. (Depth) is required.
- the speaker 100 according to the present embodiment is further reduced in thickness in the following points.
- a voice coil 1006 is connected to the end of the diaphragm 1008 in the depth direction via a voice coil bobbin 1005. That is, the voice coil bobbin 1005 and the voice coil 1006 are arranged in a state in which the voice coil bobbin 1005 and the voice coil 1006 are suspended from the magnetic circuit by the edge 1010 and the damper 1007 so as to vibrate.
- a magnetic circuit composed of the magnet 1001 and the like is disposed further inside the voice coil 1006 (lower part in FIG. 21B).
- the thickness of the diaphragm 1008, the voice coil bobbin 1005, the voice coil 1006, the magnetic circuit including the magnet 1001, and the like is the thickness of the speaker.
- the through-hole 180 is provided in the diaphragm 110, and the voice coil 120 and the voice coil bobbin 130 are disposed inside the diaphragm 110. Further, since the magnetic circuit 140 is disposed inside the voice coil bobbin 130, each component is not stacked in the thickness direction of the speaker 100, but the connection surface of the diaphragm 110 is the center plane (X-- in FIG. 1B). X ′ plane) is arranged so as to overlap each other in a nested manner. For this reason, compared with the conventional speaker, a very thin speaker can be implement
- the thickness of the speaker 100 is 1 ⁇ 2 of the thickness of the voice coil bobbin 130 on the upper side in the vibration direction and 1 ⁇ 2 of the thickness of the voice coil bobbin 130 on the lower side in the vibration direction with respect to the XX ′ plane in FIG. 1B.
- the voice coil bobbin 130 can be configured to 7 mm and the frame thickness can be 2.0 mm, and the thickness of the speaker 100 can be 11 mm in total.
- Rolling is abnormal vibration that attempts to rotate the diaphragm.
- the voice coil 120 of the speaker 100 is disposed inside the annular cross section of the diaphragm 110 and on the center plane (X-X ′ plane in FIG. 1B) of the diaphragm 110 orthogonal to the vibration direction. Further, the fixed point of the edge 150 on the frame 160, the center of gravity of the diaphragm 110, and the center of gravity of the magnetic circuit 140 are also arranged on this center plane (X-X 'plane in FIG. 1B). With this arrangement, the position of the center of gravity of the vibration system and the position of the fixing point of the support system are on the same plane, and a speaker having excellent rolling resistance can be obtained.
- the speaker 100 has an elongated structure, it is possible to reduce the thickness of the entire speaker while realizing improved rigidity by imparting characteristics to the shape of the diaphragm and the overall configuration of the speaker. And the characteristic of this speaker whole structure also produces the further effect of suppressing abnormal vibration and improving rolling resistance.
- the speaker 200 is characterized in that, in addition to the speaker 100 of the first embodiment, a voice coil lead wire is fixed inside the diaphragm 110.
- FIG. 9A is a top view showing the speaker 200.
- FIG. 9B is a schematic cross-sectional view of FIG. 9A cut in the longitudinal direction. 9A and 9B do not show the upper diaphragm 111a in the diaphragm 110.
- FIG. A grommet 201 is caulked at the longitudinal end portion of the lower diaphragm 111b, and is integrated with the lower diaphragm 111b.
- a conductive wire 203 is fixed to the eyelet 201, and the opposite end of the conductive wire 203 is connected to a terminal (not shown) provided on a frame (not shown), and a signal for driving a speaker is inputted.
- a gold thread wire can be used as the conductive wire 203.
- the voice coil 120 is fixed via a voice coil bobbin 130 on the longitudinal center line of the diaphragm 111b.
- the lead wire 202 of the voice coil 120 is fixed on the inner surface of the diaphragm 111b.
- the lead line 202 is electrically connected to the conductive line 203 connected to the eyelet 201.
- the diaphragm 111b subjected to the wiring process and the diaphragm 111a are bonded to form a cylindrical shape, thereby realizing the speaker 200 having the same magnetic circuit and frame configuration as in the first embodiment.
- the drive signal input to the terminal of the frame 160 is provided to the voice coil 120 from the lead wire 202 via the conductive wire 203 and one eyelet 201, and to the other eyelet 201, the conductive wire 203 and the frame 160 via the lead wire 202. Constitutes the electrical circuit leading to the terminal. Therefore, the voice coil 120 generates a force corresponding to the speaker input signal and vibrates the diaphragm 110. Since the lead wire 202 is fixed to the inner surface of the vibration plate 111b, when the vibration plate 110 operates, the lead wire 202 vibrates integrally with the vibration plate 110.
- FIG. 10A is a top view of the speaker 300 according to the present embodiment.
- 10B is a schematic cross-sectional view taken along the line GG ′ in FIG. 10A and viewed from the direction of the arrow g.
- speaker 300 uses diaphragm 210 having two through holes 180, and voice coil bobbins via each of two through holes 180. 130 is fixed.
- the driving position is set in consideration of the band of the speaker.
- one voice coil 1006 or voice coil 120 is arranged with the center in the longitudinal direction of the diaphragm 1008 or 110 as a driving point.
- the above structure may be used. In this case, the diaphragm is subjected to piston vibration up to the first resonance frequency.
- the speaker 300 is provided with two drive points (voice coils) in order to suppress the first resonance mode that occurs first and to achieve a flat characteristic up to the second resonance mode that occurs next.
- the driving point for controlling the primary resonance mode may be provided at the node of the primary resonance mode.
- the position of the node of the primary resonance mode in the longitudinal direction of the diaphragm 210 is 0.224 and 0.776 from the longitudinal end of the diaphragm 210 when the longitudinal length of the diaphragm 210 is 1.
- the corresponding position That is, the voice coil bobbin 130 is 0 from the longitudinal end of the diaphragm 110 when the position of the first resonance mode in the longitudinal direction of the diaphragm 210, that is, when the longitudinal length of the diaphragm 110 is 1. .. It is advisable to fix at positions corresponding to 224 and 0.776.
- the band is expanded to about four times the frequency. In the case of FIG. 8, the first resonance mode is suppressed, and the frequency can be expanded to the frequency of the next second resonance mode. Therefore, according to the present embodiment, the reproduction frequency can be increased as compared with the first embodiment.
- the speaker 300 according to the present embodiment realizes expansion of the reproduction frequency band by the number of driving points, and thus does not affect the thickness of the speaker.
- FIG. 11A is a top view of the speaker 400 according to the present embodiment.
- FIG. 11B is a schematic cross-sectional view taken along the line HH ′ in FIG. 11A and viewed from the direction of the arrow h.
- Speaker 400 uses speaker 310 having four through holes 180 to provide two more voice coil bobbins 130 in speaker 300 according to the third embodiment, and voice is transmitted through each of four through holes 180.
- the coil bobbin 130 is fixed.
- the band is further expanded.
- x1 0.130
- x2 0.37775
- FIG. 12A shows the sound pressure frequency characteristics when the position of the node of the primary resonance mode is driven (two-point drive).
- FIG. 12B shows the sound pressure frequency characteristics when the four voice coils are positioned to suppress both the primary and secondary resonance modes (4-point drive).
- FIG. 12C shows a sound pressure frequency characteristic when the center drive is performed. Comparing FIG. 12A, FIG. 12B, and FIG. 12C, it can be seen that the resonance mode is suppressed and the reproduction frequency band is expanded by devising the number and position of drive points.
- the speaker 400 according to the present embodiment like the speaker 300 according to the third embodiment, realizes expansion of the reproduction frequency band by the number of drive points, and thus does not affect the thickness of the speaker.
- FIG. 13 is a perspective view showing a magnetic circuit 540 used in the speaker 500.
- FIG. 14 is a cross-sectional view of the speaker 500 in the short direction.
- the magnetic circuit 540 has a structure in which an auxiliary plate 401 that goes around both sides of the joint surface 143 of the magnet 141 is further arranged in the magnetic circuit 140 according to the first embodiment.
- the auxiliary plate 401 is bonded to the end surface of one plate 142 and is disposed so as to wrap around the both sides of the bonding surface 143 of the magnet 141 outside the diaphragm 110.
- letters N and S are shown in FIG.
- the polarities of N and S are repulsive polarities and have a reversible relationship.
- the flow of magnetic flux is indicated by a broken line arrow.
- the generated magnetic flux exits from the joint surface 143 of one magnet 141 in the horizontal direction, and then reaches the plate 142 while repelling the magnetic flux emitted from the other magnet 141.
- the auxiliary plate 401 constitutes a magnetic circuit.
- the magnetic flux generated from the magnet 141 reaches the auxiliary plate 401 after leaving the bonding surface 143 in the horizontal direction.
- the magnetic flux travels through the auxiliary plate 401 and reaches the plate 142. For this reason, the magnetic flux of a component perpendicular
- a driving force is generated in the voice coil 120 by the applied current and a magnetic field generated by the magnetic circuit.
- the generated driving force is transmitted to the diaphragm 110 via the voice coil bobbin 130.
- the diaphragm 110 to which the driving force is transmitted vibrates to emit sound into the space.
- the magnetic flux interlinking with the voice coil 120 increases, it is possible to realize a speaker capable of reproducing a loud sound with higher sound pressure. That is, by making good use of the structure in which the magnetic circuit is embedded in the diaphragm and arranging the auxiliary plate 401, the magnetic flux can be increased and the sound pressure can be improved without increasing the space.
- FIG. 15 is a perspective view showing a magnetic circuit 640 used in the speaker 600.
- FIG. 16 is a cross-sectional view of the speaker 600 in the short direction.
- FIG. 17 is an overview diagram showing the component configuration of the speaker 600.
- the magnetic circuit 640 has a structure in which auxiliary magnets 601 are further arranged on both sides of the joint surface 143 of the magnet 141 in the magnetic circuit 140 according to the first embodiment.
- the auxiliary magnet 601 is fixed to the frame 160 on the side surface of the joint surface 143 at a position separating the diaphragm 110.
- the auxiliary magnet 601 is magnetized in a direction perpendicular to the magnet 141 and the bonding surface 143 is magnetized to the N pole
- the auxiliary magnet 601 is magnetized so that the S pole is in the direction of the bonding surface 143.
- 143 is an S pole
- it is magnetized so that the N pole is in the direction of the joint surface 143.
- the letters N and S are shown in FIG.
- the polarities of N and S are repulsive polarities and have a reversible relationship.
- the flow of magnetic flux is indicated by broken line arrows.
- the generated magnetic flux comes out from the joint surface 143 of the magnet 141 in the horizontal direction, and then the magnetic flux emitted from the auxiliary magnet 601 is added to reach the plate 142 while repelling each other. For this reason, the magnetic flux of a component perpendicular
- a driving force is generated in the voice coil 120 by the applied current and a magnetic field generated by the magnetic circuit.
- the generated driving force is transmitted to the diaphragm 110 via the voice coil bobbin 130. Sound is radiated into the space when the diaphragm 110 to which the driving force is transmitted vibrates.
- the magnetic flux interlinking with the voice coil 120 increases, it is possible to realize a speaker capable of reproducing a loud sound with higher sound pressure. That is, by making good use of the structure in which the magnetic circuit is embedded in the diaphragm and arranging the auxiliary magnet 601, the magnetic flux can be increased and the sound pressure can be improved without increasing the space. Further, similarly to the fourth embodiment, the auxiliary plate 401 may be provided, and the auxiliary magnet 601 may be provided on the auxiliary plate 401. Thereby, without increasing the space, the magnetic flux can be further increased, and the sound pressure can be improved.
- Embodiments 1 to 6 have been described as examples of implementation in the present disclosure. However, the present disclosure is not limited to this, and can also be applied to embodiments in which changes, replacements, additions, omissions, etc. are made as appropriate.
- the speakers described in Embodiments 1 to 6 can be easily thinned, they can be used for electronic devices such as thin televisions, mobile phones, and PDAs. That is, the electronic device can be configured to include a speaker according to the present disclosure and a housing that holds the speaker inside. Therefore, other embodiments will be exemplified below.
- FIG. 18 shows a mobile information terminal device 701 equipped with a speaker selected from those shown in the first to sixth embodiments of the present disclosure.
- reference numeral 702 denotes a screen
- 700 denotes a speaker selected from those shown in the first to sixth embodiments.
- the speakers 700 are arranged at three locations, but any number of speakers may be used as long as one or more speakers are provided. If there is only one speaker device, it will be monaural. If two or more speakers are used, it can be used as a device for sound field control or HRTF.
- the speaker 700 By mounting the speaker 700 on a device having a limited mounting volume, such as the mobile information terminal device 701, wide-band reproduction can be stably performed even with a limited volume.
- the diaphragm may be directed to the sound hole side or the frame may be directed to the sound hole side with respect to the sound hole provided in the housing.
- FIG. 19 shows an image display device 801 equipped with a speaker selected from those shown in the first to sixth embodiments of the present disclosure. More specifically, the image display device 801 is a PC, a thin TV, or the like.
- reference numeral 202 denotes a screen
- 800 denotes a speaker selected from those shown in the first to sixth embodiments.
- the speakers 800 are arranged at a total of 16 locations, but any number of speakers 800 may be used as long as one or more speakers 800 are provided. If one unit is monaural, two units are stereo, and if two or more units are used (for example, arranged as a line array), it can be used as a device for sound field control or HRTF.
- the diaphragm may be directed to the sound hole side or the frame may be directed to the sound hole side with respect to the sound hole provided in the housing.
- FIG. 20 shows a mounting diagram of the on-vehicle speaker.
- reference numeral 901 denotes an automobile door
- 900 denotes a speaker selected from those shown in the first to sixth embodiments of the present disclosure.
- the speakers 900 are arranged at three locations, but any number of speakers 900 may be used as long as the number is one or more.
- FIG. 20 shows an example in which the vehicle is attached to the door 901 of the automobile, but it may be attached to any position of the automobile such as a dashboard, pillar, seat, headrest, or ceiling of the automobile. In addition to automobiles, they may be attached to various moving means such as trains, monorails, linear motors, airplanes, and ships.
- the speakers shown in the first to sixth embodiments of the present disclosure can realize a thinner speaker than conventional speakers.
- the entire moving means is reduced in size, and the comfort can be improved by increasing the living space.
- the diaphragm may be directed to the sound hole side or the frame may be directed to the sound hole side with respect to the sound hole provided in the housing.
- the speaker according to the present disclosure can be used for electronic devices such as flat-screen TVs, mobile phones, and PDAs.
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- Engineering & Computer Science (AREA)
- Physics & Mathematics (AREA)
- Acoustics & Sound (AREA)
- Signal Processing (AREA)
- Multimedia (AREA)
- Audible-Bandwidth Dynamoelectric Transducers Other Than Pickups (AREA)
- Diaphragms For Electromechanical Transducers (AREA)
- Details Of Audible-Bandwidth Transducers (AREA)
Abstract
Description
この創案に基づいた本開示の様々な態様は、次の通りである。
以下、実施の形態1について説明する。まずは、本実施の形態におけるスピーカ100の構成について説明する。図1Aは、本実施形態に係るスピーカ100の上面図である。また、図1Bは、図1AにおけるA-A’線で切断し、矢印aの方向から見た概略断面図である。また、図1Cは、図1AにおけるB-B’線で切断し、矢印bの方向から見た概略断面図である。
以下、実施の形態2に係るスピーカ200について説明する。スピーカ200は、実施の形態1のスピーカ100に加え、ボイスコイル引き出し線を振動板110内部に固着したことを特徴とする。
以下、実施の形態3について説明する。図10Aは、本実施形態に係るスピーカ300の上面図である。また、図10Bは、図10AにおけるG-G’線で切断し、矢印gの方向から見た概略断面図である。
以下、実施の形態4について説明する。図11Aは、本実施形態に係るスピーカ400の上面図である。また、図11Bは、図11AにおけるH-H’線で切断し、矢印hの方向から見た概略断面図である。
以下、実施の形態5に係るスピーカ500について説明する。図13は、スピーカ500に用いる磁気回路540を示す斜視図である。また、図14は、スピーカ500の短手方向の断面図である。
以下、実施の形態6に係るスピーカ600について説明する。図15は、スピーカ600に用いる磁気回路640を示す斜視図である。また、図16は、スピーカ600の短手方向の断面図である。また、図17は、スピーカ600の部品構成を示す概観図である。
さらに、本開示における実装の例示として、実施の形態1~6を説明した。しかしながら、本開示は、これに限定されず、適宜、変更、置き換え、付加、省略などを行った実施の形態にも適用可能である。また、上記実施の形態1~6で説明したスピーカは、薄型化が容易であるので、薄型テレビや携帯電話やPDAなどの電子機器などに利用することができる。すなわち、電子機器は、本開示に係るスピーカと、スピーカを内部に保持する筐体とを備える構成とすることが可能である。そこで、以下、他の実施の形態を例示する。
110、111a、111b、210、310、610 振動板
112 張り合わせ部
120 ボイスコイル
130 ボイスコイルボビン
140、540、640 磁気回路
141 マグネット
142 プレート
143 接合面
150 エッジ
160 フレーム
170 ダストキャップ
180 貫通孔
202 引き出し線
203 導電線
401 補助プレート
601 補助マグネット
701 モバイル情報端末装置
702 画面
801 画像表示装置
901 自動車のドア
Claims (14)
- 細長構造のスピーカであって、
フレームと、
振動方向と垂直な平面の形状が長手と短手を有する縦長の形状で、中空構造である振動板と、
前記振動板を振動可能に支持し、前記フレームに固定されるエッジと、
前記振動板を貫通して、接続される少なくとも1つの筒形状のボイスコイルボビンと、
前記振動板の中空構造の内部で、前記ボイスコイルボビンに固着されるボイスコイルと、
前記ボイスコイルボビンの内部に、前記ボイスコイルを駆動させるための磁気回路とを備えることを特徴とする、スピーカ。 - 前記ボイスコイルは、前記ボイスコイルボビンの高さを2等分する位置に配置されるように固着されることを特徴とする、請求項1に記載のスピーカ。
- 前記ボイスコイルの重心と、前記エッジの前記フレームへの固定点と、前記振動板の重心と、前記磁気回路の重心とが、同一平面上に配置されることを特徴とする、請求項2に記載のスピーカ。
- 前記振動板の長手方向の終端部にハトメがかしめられており、
前記ハトメと前記フレームに設けたターミナルを接続する導電線と、
前記ハトメから前記ボイスコイルに接続された引き出し線とをさらに備え、
前記引き出し線は、振動板内部に固着されていることを特徴とする、請求項1に記載のスピーカ。 - 前記磁気回路は、2つのマグネットを反発する方向に固着した構成を含むことを特徴とする、請求項1に記載のスピーカ。
- 前記振動板の短手方向の断面形状が、円形状、長円形状、中空台形または中空多角形であることを特徴とする、請求項1に記載のスピーカ。
- 前記ボイスコイルボビンを2つ備え、
前記ボイスコイルボビンは、前記振動板の前記長手方向の第1次共振モードの節の位置に1つずつ配置されることを特徴とする、請求項1に記載のスピーカ。 - 前記振動板の長手方向の一端を0とし、他端を1としたときに、
前記ボイスコイルボビンは、0.224と、0.776とに相当する位置に配置されることを特徴とする、請求項7に記載のスピーカ。 - 前記ボイスコイルボビンを4つ備え、
前記ボイスコイルボビンは、前記振動板の長手方向の第1次共振モードおよび第2次共振モードの節の位置に配置されることを特徴とする、請求項1に記載のスピーカ。 - 前記振動板の長手方向の一端を0とし、他端を1としたときに、
前記ボイスコイルは、0.1130と、0.37775と、0.62225と、0.8870との位置に配置されることを特徴とする、請求項1に記載のスピーカ。 - 前記振動板の外側に、前記振動板の長手方向における前記磁気回路の両側を回り込むような補助プレートをさらに備えることを特徴とする、請求項1に記載のスピーカ。
- 前記振動板を隔てた位置であって、前記振動板の長手方向における前記磁気回路の両側に補助マグネットをさらに備える、請求項1に記載のスピーカ。
- 前記振動板は、前記長手方向両端の形状が、半球形状である、請求項1に記載のスピーカ。
- 請求項1に記載のスピーカを備える、電子機器。
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CN201280005778.0A CN103329572B (zh) | 2011-11-24 | 2012-10-23 | 扬声器及具备扬声器的电子设备 |
US13/977,967 US9106992B2 (en) | 2011-11-24 | 2012-10-23 | Loudspeaker and electronic equipment including the loudspeaker |
JP2013545767A JP5950261B2 (ja) | 2011-11-24 | 2012-10-23 | スピーカおよびスピーカを備えた電子機器 |
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PCT/JP2012/006766 WO2013076914A1 (ja) | 2011-11-24 | 2012-10-23 | スピーカおよびスピーカを備えた電子機器 |
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US (1) | US9106992B2 (ja) |
JP (1) | JP5950261B2 (ja) |
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Cited By (1)
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JP2017212713A (ja) * | 2016-05-26 | 2017-11-30 | エーエーシー テクノロジーズ ピーティーイー リミテッドAac Technologies Pte.Ltd. | スピーカー |
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- 2012-10-23 WO PCT/JP2012/006766 patent/WO2013076914A1/ja active Application Filing
- 2012-10-23 US US13/977,967 patent/US9106992B2/en active Active
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US9106992B2 (en) | 2015-08-11 |
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JPWO2013076914A1 (ja) | 2015-04-27 |
CN103329572A (zh) | 2013-09-25 |
CN103329572B (zh) | 2016-10-12 |
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