The present invention relates to a damper for a speaker and a speaker device.
A damper for a speaker is formed as an annular member, a voice coil is connected to the inner periphery side thereof, and the outer periphery side is connected to a static part such as a frame, whereby the static part supports the voice coil. The damper for a speaker supports the voice coil in magnetic space (magnetic gap) of a magnetic circuit. The voice coil is vibratably held in the axis direction when a speaker is driven, and the voice coil is held at a given position in the magnetic space when the speaker is not driven. Further, the damper for a speaker is required to regulate the vibration of the voice coil in one axis direction such that the rolling is restrained, and thus a double damper for double supporting the voice coil is proposed as an effective structure for this purpose (for example, see patent literature 1 described below).
[Patent literature 1] Microfilm of Utility model application 1-109831 (Laid-open utility model publication 3-49000)
The damper for a speaker has an elastically expandable and contractable structure in a direction crossing the circumferential direction of the annular member. Originally, an elastic restoring force of the damper for a speaker is applied in a direction opposite the vibration of the voice coil, whereby a large load is applied in response to the amount of the amplitude of vibration and thus the amplitude of vibration is suppressed. The aforementioned double damper structure has a high restraining effect against the rolling of the voice coil, however the load applied to the amplitude of vibration is doubled compared to that of a single damper, which may unfavorably reduce the driving efficiency of the voice coil.
In order to improve the driving efficiency of a voice coil, the elastic restoring force of the damper for a speaker may be lowered (softened) (may have higher compliance). However, this may cause the rigidity of the connecting part between the damper for a speaker and the static part to decrease, thereby reducing a supporting strength of the damper for a speaker itself, and thus the function of regulating the vibration of the voice coil in one axis direction is deteriorated. Further, since a vibration suppressing force against an excessive amplitude of vibration is not sufficiently obtained, when the voice coil vibrates with an excessive amplitude of vibration, a too much stress is applied to the inner periphery part of the damper that is the connecting part between the damper of a speaker and the voice coil and thus the problems such as the peel-off and the breakage of the damper may occur. In order to regulate the vibration of the voice coil in one axis direction and to suppress an excessive vibration of the voice coil, the rigidity of the damper is required to improve to some extent (low compliance).
Meanwhile, since the displacement of the damper for a speaker does not monotonically increase in accordance with the amplitude of vibration of the voice coil, reproduction with high linearity is difficult to achieve. When the rigidity of the damper for a speaker is increased to some extent, since the compliance of the damper is comparatively small, linearity is decreased even when the voice coil vibrates with comparatively small amplitude of vibration. In order to improve linearity when the voice coil vibrates with comparatively small amplitude of vibration, the compliance of the damper is required to be comparatively large. However, in view of the situation where the voice coil vibrates with comparatively large amplitude of vibration, there is little choice but to improve the rigidity of damper to some extent and decrease the compliance as described above.
One or more embodiments of the present invention is provide a damper for a speaker having both high compliance and low compliance, to improve a driving efficiency of the voice coil while regulating the vibration in one axis direction, to obtain a vibration suppressing force against excessive vibration while securing a supporting force of the damper for a speaker, and to restrain the peel-off or breakage of the damper when large amplitude of vibration is applied while enabling reproduction with high linearity in the practical region of the amplitude of vibration.
One or more embodiments of the present invention are provided with the following configurations.
A damper for a speaker that vibratably supports a voice coil to a static part. The damper for a speaker includes a first damper and a second damper. The first damper and the second damper are formed in an annular shape having an inner periphery part and an outer periphery part respectively, the first and second dampers being formed in a shape expandable and contractable in a direction crossing the circumferential direction of the annular shape. The inner periphery part of the second damper is connected to the first damper between the inner periphery part and the outer periphery part of the first damper, and each outer periphery part of the first damper and the second damper is connected to each other such that annular space is formed between the first damper and the second damper. The first damper includes a plurality of expandable and contractable curved parts formed at least from the connecting point of the inner periphery part of the second damper to the inner periphery part of the first damper in a direction crossing the circumferential direction.
FIGS. 1(A)-(C) are partial cross-sectional views of a damper for a speaker according to an embodiment of the present invention (partial cross-sectional view illustrating only one side of a center axis O);
FIGS. 7(A)-(D) are views illustrating another forming example of a damper for a speaker according to an embodiment of the present invention;
FIGS. 13(A)-(D) are views illustrating a planar shaped example of a damper for a speaker according to an embodiment of the present invention (schematic plan view);
Hereinafter, embodiments of the present invention are described. The embodiments of the present invention include what are shown in the drawings, but are not limited to only these examples. In the description of the embodiments of the present invention, upper and lower sides are indicative of the sound emission direction and the direction opposite the sound emission direction. A damper (10) for a speaker according to an embodiment of the present invention is a damper for a speaker for vibratably supporting a voice coil to a static part, including a first and a second dampers (11, 12) that are formed in an annular shape having an inner periphery part (11a, 12a) and an outer periphery part (11b, 12b), being formed in an expandable and contractable shape in a direction crossing the circumferential direction of the annular member, and the inner periphery part (12a) of the second damper (12) is connected to the first damper (11) between the inner periphery part (11a) and the outer periphery part (11b) of the first damper (11), and each outer periphery part (11b. 12b) of the first damper (11) and the second damper (12) are connected to each other, whereby annular space (S) is formed between the first damper (11) and the second damper (12), and a plurality of expandable and contractable curved parts (11c) are formed in the first damper (11) at least from the connecting point of the inner periphery part (12a) of the second damper (12) to the inner periphery part (11a) of the first damper (11) in a direction crossing the circumferential direction.
The static part so called here is a collective term of parts that support the vibration by the voice coil. The voice coil or vibrating bodies that are vibrated by the voice coil vibrate relative to the static part. The static part itself is not intended to be completely static here and the entire part of the static part may be vibrated or moved by receiving the effect of the vibration of the voice coil or receiving other forces.
The voice coil is a coil shaped conductive wire through which an audio signal (voice currents) flows and the damper (10) for a speaker supports the voice coil to the static part directly or via other members (voice coil support part and so forth). The damper (10) for a speaker according to an embodiment of the present invention includes the first damper (11) and the second damper (12), however the number of dampers is not limited to two, and three or more dampers may be included. As least the first damper (11) and the second damper (12) are formed in an annular shape, and the inner periphery part (11a, 12a) is formed on the inside thereof and the outer periphery part (11b, 12b) is formed on the outside thereof. Further, the first damper (11) and the second damper (12) are formed in an expandable and contractable shape in a direction crossing the circumferential direction of the annular member. The term of “expandable and contractable” means that the distance from the inner periphery part to the outer periphery part of the damper become large or small, including the deformation of the damper. Further, the expandable and contractable shape includes a so-called corrugation shape. The vibration of the voice coil causes the first damper (11) and the second damper (12) to expand and contract, thereby allowing the voice coil to vibrate.
The inner periphery part (12a) of the second damper (12) is connected to the part between the inner periphery part (11a) and the outer periphery part (11b) of the first damper (11). Further, the outer periphery part (11b) of the first damper (11) and the outer periphery part (12b) of the second damper (12) are connected to each other. At this point, the annular space is formed between the first damper (11) and the second damper (12) such that both dampers do not closely contact with each other as a whole, and each damper is configured to be independently expandable and contractable. As such, when the first damper (11) mainly acts, the second damper (12) has little effect on the action.
And, a plurality of expandable and contractable curved parts (11c) are formed at the first damper (11) at least from the connecting point of the inner periphery part (12a) of the second damper (12) to the inner periphery part (11a) of the first damper (11) in a direction crossing the circumferential direction. That is, the first damper (11) can be configured to obtain a structure with large compliance, having a plurality of curved parts (11c) formed on the inner side portion thereof, which receives little effect from the second damper (12).
Hereinafter, a configuration example of a damper for a speaker according to an embodiment of the present invention is described with reference to the drawing.
In each example shown in
In the aforementioned description, the curved part means a part which has a cross-section formed in an arc shape or corrugation shape. A plurality of curved parts means a part which has a cross-section having a plurality of curved top parts. Further, the curved parts are formed in substantially similar shape in the circumferential direction of the annular member, and are formed in substantially similar curved shape or corrugation shape anywhere in the cross-section in a direction orthogonal to the circumferential direction.
Another example of the curved part having a curved top part includes, for example, a V-shape curved part constituted by two linear portions and a curved top part that is formed by crossing the two linear portions. Further in the example shown in the drawing, the curved top part is provided in the proximity of the center position of the curved part. However the curved top part may be provided at the position displaced toward the inner periphery side or the outer periphery side with respect to the center position. Moreover, it is only necessary that the curved part is formed in a mountain like shape, for example, the curved top part may be formed in a flat shape as is the flat part of the first damper 11C shown in
The damper 10 for a speaker includes the first damper 11 on the side of the inner periphery part and the second damper 12 on the side of outer periphery part with the connecting point as a boundary between the inner periphery part of the second damper 12 and the first damper 11, and the first damper 11 is configured to be more flexible and movable (higher compliance) whereas the second damper 12 is configured to have higher rigidity (lower compliance) than the first damper 11, whereby an effective function can be obtained as described below.
According to this configuration, the flexible first damper 11 on the inner periphery side mainly moves in the practical amplitude of vibration (for example, the amplitude of vibration of the voice coil is comparatively small in the use of the reproduction of music with a normal sound volume) and the second damper 12 assists the support of the first damper 11 from the outer periphery side. In this case, the displacement of the first damper 11 is monotonically increased within the practical amplitude of vibration in response to the vibration of the voice coil, whereby reproduction with high linearity can be achieved.
Further, when the vibration of the voice coil enters into the domain of the greater amplitude of vibration beyond the domain of the practical amplitude of vibration, for example, in response to large voice currents being inputted to a speaker, the first damper 11 on the inner periphery side starts to produce tension (starts to extend completely), and thereby the second damper 12 on the outer periphery side starts to move gradually. Within the domain of this greater amplitude of vibration, linearity is reduced while the second damper 12 with low compliance functions such that the braking against an excessive vibration is applied to the voice coil to restrain damages (peel-off, breakage, etc.) of the connecting point between the outer periphery parts 11b, 12b of the first damper 11 and the second damper 12, and the static part. Also, in the sound quality, a saturated feeling in audibility can be alleviated (soft distortion).
As such, the damper a speaker 10 can be configured such that the inner periphery side is flexible by the first damper 11 while the outer periphery side is reinforced by the second damper 12, and therefore the voice coil can be vibrated at high efficiency of vibration with high linearity within a practical amplitude range of vibration while the tension applied to the first damper is reduced by the function of the second damper 12 with low compliance with respect to the greater amplitude of vibration in response to the greatest voice currents being inputted, in other words, the acceleration of the first damper is prevented from being comparatively large. That is, the damper 10 for a speaker can have both high compliance to improve linearity and high input resistance. In the conventional damper, if high compliance is pursued to improve linearity, resistance strength when the greater amplitude of vibration is applied is reduced, and thus high input resistance cannot be obtained.
Further, as a feature of the damper 10 for a speaker, the second damper 12 is connected only on the outer periphery side of the first damper 11 to reinforce the first damper 11. When the voice currents become large such that the amplitude of vibration of the voice coil becomes large, the second damper 12 with low compliance connected to the outer periphery side starts to extend gradually after the first damper 11 with high compliance that is on the inner periphery side completely extends, and thus the impact on the connecting part between the damper 10 and the voice coil (or voice coil support part) or the connecting part between the damper 10 for a speaker and the static part due to a dramatic change in acceleration can be alleviated. As such, the mechanical fatigue applied on the aforementioned connecting part can be restrained.
Further, the damper 10 for a speaker is configured such that the inner periphery part 12a of the second damper 12 is connected to the first damper 11 between the inner periphery part 11a and the outer periphery part 11b of the first damper 11 and each of the outer periphery parts 11b, 12b of the first damper 11 and the second damper 12 is connected to each other such that the annularly shaped space S is formed between the first damper 11 and the second damper 12. As such, the annular space S improves the torsional rigidity of the damper 10 for a speaker and thus the capability of regulating the vibration of the voice coil in one axis direction can be strengthened and the rolling of the voice coil and so forth can be restrained. As such both the improvement of driving efficiency due to the first damper 11 with high compliance and the regulation of the vibration of the voice coil in one axis direction can be achieved.
Further the annular space S may or may not be a sealed space to the outside. In order to form the annular space S that is not sealed to the outside, for example, the first damper 11 and the second damper 12 are formed with a member that has a ventilation characteristic or a vent hole is formed in a part of the first damper 11 or the second damper 12 such that the annular S is communicated with the outside.
The shape of the first damper 11 is formed such that a plurality of expandable and contractable curved parts 11c are provided at least from the connecting point of the inner periphery part 12a of the second damper 12 to the inner periphery part 11a of the first damper 11 in a direction crossing the circumferential direction, whereby higher compliance can be easily achieved. The first damper 11 is continuously formed with one member from the inner periphery side 11a to the outer periphery side 11b, whereby manufacturing becomes easier with simple structure and at low cost. The first damper 11 can adopt the shape of the conventional high compliance damper as is.
On the one hand, the second damper 12 is required to have a damper function expandable and contractable in a direction crossing the circumferential direction of the annular member. As such the configuration and function are different from a damper in which a rigid reinforcing material that is unexpandable and uncontractable is connected on the outer peripheral side. The second damper 12 has an expandable and contractable function in a direction crossing the circumferential direction of the annular member, whereby a damper function is gradually effected with the magnitude of the vibration of the voice coil and braking in the greater amplitude of vibration is gradually effected, and thus the aforementioned soft distortion can be obtained.
The second damper 12 may have a shape such that a plurality of expandable and contractable curved parts 12c (12c1,12c2) are formed in a direction crossing the circumferential direction of the annular member as shown in
Further, in the second damper 12, the curvature diameter of the curved part 12c2 on the outer periphery side is formed so as to be larger than the curvature diameter of the curved part 12c1 on the inner periphery side, whereby the compliance on the outermore periphery side can be large, and as such, the magnitude relation can be arbitrarily adjusted between the compliance on the outer periphery side and the compliance on the inner periphery side.
Further, the outer periphery part of the first damper 11 which forms the annular space S with the second damper 12 becomes the part which does not require high compliance by being connected to the second damper 12. As such also in the first damper 11, a plurality of curved parts 11c is formed such that the curvature diameter of the curved part on the outer periphery side is larger than the curvature diameter of the curved part on the inner periphery side by changing one curvature part 11c, whereby the compliance on the outermore periphery side can be improved.
The inner periphery part 12a of the second damper 12 is formed along the surface profile of the first damper 11. As such, the inner periphery part 12a of the damper 12 can be in contact with and connected to the middle portion (a part) of the first damper 11 that has curved parts 11c. Further, the inner periphery part 12a of the damper 12 is in contact with the middle portion (a part) of the first damper 11, whereby the first damper 11 operates simultaneously with the second damper 12 in the connecting part, thereby following the vibration of the voice coil. Further, the middle portion of the first damper 11 and the inner periphery part 12a of the second damper 12 are formed substantially in the same shape, whereby a stress can be uniformly applied to the entire connecting part, thus the occurrence of peel-off and so on can be restrained. In the examples shown in
As shown in each example in
Further, the hardness of the first damper 11 and the second damper 12 is adjusted in accordance with the aforementioned connecting position, whereby the inflection point of stiffness curve in small input (when the amplitude of vibration of the voice coil is small) and in large input (when the amplitude of vibration of the voice coil is large) can be arbitrarily set. If the compliance of the first damper 11 is set higher (flexibility is high), the linearity in small input can be improved, and if the aforementioned connecting position is shifted more outer side such that the valid length of the first damper 11 is high, the driving domain where compliance is large (move flexibly) can be extended.
In each example of
As shown in each example in
The symmetric property of vertical vibration in stiffness is improved if the position of the inner periphery part 12a of the second damper 12 is shifted upwardly (on the curved projecting side of the second damper 12) under the assumption that the second damper 12 is connected on the upper side of the first damper 11, projecting upwardly. The asymmetric property of vertical vibration in stiffness (asymmetrical property between the stiffness curve when the voice coil vibrates upwardly and the stiffness curve when the voice coil vibrates downwardly) becomes large if the position of the inner periphery part 12a of the second damper 12 is shifted downwardly (opposite the curved projecting side of the second damper 12).
The damper 10 for a speaker has asymmetrical property normally in a vertical action, however if the structure of the second damper 12 is adjusted by adopting the structure of joining two different shaped dampers (the first damper 11 and the second damper 12) such that a braking force is applied in a direction the first damper 11 excessively extends on the basis of a specific characteristic of the first damper 11 as a single formed item, the asymmetrical property of vertical vibration in stiffness can be improved. For example, as shown in
On the contrary, by using the asymmetrical property of vertical vibration in stiffness the lower side vibration of the voice coil is suppressed, thereby a bottom hit against a yoke and so forth of a magnetic circuit due to the lower amplitude of vibration of the voice coil can be restrained. As shown in the examples in
The material of the damper 10 for a speaker is now described. Since the damper 10 for a speaker is configured such that the second damper 12 supports the first damper 11, the mass of the first damper 11 substantially has a large contribution on the equivalent mass of a vibration system when the voice coil vibrates with a comparatively small amplitude of vibration (within the domain of the practical amplitude of vibration). In order to form the first damper 11 having a high compliance, the first damper 11 is preferably formed with a member having comparatively small density with pores formed therein, such as a fiber system member including a cloth having, for example, unwoven fabric or woven fabric that are composed of fiber. Further, as unwoven fabric used for the fiber system member (cloth), for example, what has comparatively large area density with comparative large number of punching by a needle punch or what is composed of fiber with comparatively small diameter and so forth can be preferably used. Further, as woven fabric of a fiber system member (cloth), what is composed with fiber having comparatively small diameter can be preferably used. By using such a first damper, a flexible damper with comparatively high compliance can be obtained.
When both the first damper and the second damper are formed with fibrous member, the diameter of the fiber forming the second damper 12 is formed to be larger than the diameter of the fiber forming the first damper 11, whereby the difference in compliance between the first damper 11 and the second damper 12 can be obtained such that the compliance of the second damper 12 is smaller than the compliance of the first damper. Further, when both the first damper 11 and the second damper 12 are formed with fibrous member, the area density of the fiber forming the second damper 12 is formed to be higher than the area density of the fiber forming the first damper 11, whereby the difference in compliance between the first damper 11 and the second damper 12 can be obtained such that, for example, the compliance of the second damper 12 is smaller than the compliance of the first damper.
Further, in order to improve the rigidity of the second damper 12, the rigidity of the fiber itself that forms the second damper 12 is improved by using a cloth composed of thick thread and a plurality of fibers is restrained by adhesive resin. As such the restoring force and rigidity of the second damper is improved.
In this case, the mass of the second damper 12 is comparatively large by the applied adhesive resin, however the mass increase has little effect on the equivalent mass of vibration system of a speaker within the domain of the practical amplitude of vibration, thereby causing little adverse effect such as the reduction of sensitivity (the ratio of output sound pressure to voice currents is reduced). Further, by restraining the fiber with the adhesive resin, the second damper 12 is provided with a restoring force and rupture strength while the rigidity of the adhesive resin is applied to the second damper 12, and thereby the rigidity of the second damper 12 is comparatively large. Further, the elastic force of the adhesive resin can comparatively improve the restoring force of the second damper 12 as well. By selecting the type of the adhesive resin, desired elasticity or rigidity can be applied to the second damper 12. Specifically, by impregnating a cloth with thermostatic resin such as phenol resin and adjusting the impregnated specific gravity, the elasticity or the rigidity applied to the second damper 12 can be adjusted. Further, the physical property of the second damper 12 can be adjusted, which includes adjusting the internal loss of the second damper 12 with the slip between fibers or the internal loss of the adhesive resin, hardening the adhesive resin and at the same time improving the rigidity of the second damper 12 by pressing the cloth with a heated pressing member, and so forth.
The resin layer 13 is continuously formed in the proximity of the surface of the second damper 12, desired elasticity (Young's modulus) and internal loss can be applied to the second damper 12 in accordance with a physical characteristic of the resin layer 13. Further, depending on the selected material of the resin layer 13, the rigidity that is higher than the rigidity of the selected cloth material of the second damper 12 can be applied to the second damper 12. When the resin layer 13 is formed only on the second damper 12, the vibration characteristic (for example, the aforementioned stiffness characteristic) can be improved when the second damper 12 expands and contracts in response to the large amplitude of vibration (large input) of the voice coil. Further, the resin layer 13 is continuously formed from the second damper 12 to the first damper 11, the vibration characteristic of the entire damper 10 for a speaker can be improved even in a shifting range of the amplitude of vibration of the voice coil shifting from the small amplitude of vibration (small input) to the large amplitude of vibration (large input). Particularly, by covering the connecting part between the first damper 11 and the second damper 12 with the resin layer 13, the connecting strength of the connecting part can be improved.
Further, when the fiber forming the second damper 12 is restrained by the adhesive resin, another resin layer 13 can be formed in the proximity of the surface of the second damper 12. In this case, the adhesive resin is preferably selected mainly so as to serve to adjust elasticity (Young's modulus) and the resin layer 13 that is formed in the proximity of the surface is preferably selected so as to serve to adjust the internal loss. At this point, the resin layer 13 is selected such that the internal loss of the resin material forming the resin layer 13 is larger than the internal loss of the aforementioned adhesive resin. By adopting the resin layer 13 that has higher internal loss, the unwanted vibration in the damper 10 for a speaker can be restrained, and thus a rolling phenomenon and so forth generating in the voice coil can be restrained. Further, it is possible to restrain the vibration of the voice coil from being transmitted to a frame or diaphragm that are described later via the damper 10 for a speaker, causing abnormal noise and harmonic distortion due to the unwanted vibration.
In the example shown in
A speaker wire (not shown) for inputting an audio signal from the outside to the voice coil 30 may be placed in the space surrounded by the damper 10 and the diaphragm 3. At this point by lowering the height of the curved part of the outer periphery side to be lower than the height of the curved part of the inner periphery side, for example as is the damper 10 shown in
Further, the aforementioned second damper includes a plurality of curved parts while including a single curved part with a large curvature diameter, and it can also be said that the single curved part includes a plurality of curved parts with a small curvature diameter. The virtual curved top part of the curved part with a large curvature diameter is provide on the upper side position of the curved top part of the curved part with a small curvature diameter, for example in
Further, the second damper having a plurality of curved parts with a large curvature diameter may be used without being limited to the aforementioned second damper, and thus it is possible to arbitrarily change as necessary.
In the example shown in the drawing, the magnetic circuit 20 includes a magnet 21, a yoke 22, and a plate 23. A magnetic gap 20G is formed such that the voice coil 30 is arranged between the inner surface of the yoke 22 and the outer surface of the plate 23, and the magnetic gap 20G forms magnetic space constituted by magnetic field lines crossing the conductive wire of the voice coil 30. The example shown in the drawing illustrates a so-called inner magnet type magnetic circuit, however the type of the magnetic circuit 20 is not specifically limited an inner magnet type and it may be an outer magnet type or a both magnet type consists of an inner magnet and an outer magnet.
As described above, the damper 10 for a speaker includes the first damper 11 and the second damper 12, and the inner periphery part is connected to the voice coil support part 31 (or voice coil 30) and the outer periphery part is supported by a frame 2 that is the static part. More specifically, the inner periphery part 11a of the first damper 11 of the damper 10 for a speaker is coupled to the outer surface of the voice coil support part 31, and the connecting part between the outer periphery part 11b of the first damper 11 and the outer periphery part 12b of the damper 12 is coupled to the frame 2.
In such a speaker device 1, when an audio signal is inputted into the voice coil 30, the voice coil 30 vibrates along the center axis O and thereby vibrating the voice coil support part 31 supported by the damper 10 for a speaker. Thus, the diaphragm 3 and the edge 4 vibrate thereby emitting sound toward the sound emission direction SD.
As described above, in the speaker device 1, the damper 10 for a speaker includes the first damper 11 which is formed to have high compliance and the second damper 12 which is formed to have low compliance. When the voice coil vibrates within the domain of the practical amplitude of vibration in response to a small input (when small voice currents are inputted), the speaker device 1 operates with the high compliance of the first damper 11. When the voice coil vibrates with large amplitude of vibration beyond the domain of the practical amplitude of vibration in response to a large input (when large voice currents are inputted), the speaker device 1 operates with the low compliance by synthesizing the compliances of the second damper 12 and the first damper 11.
As such, reproduction with high linearity can be achieved within the domain of the practical amplitude of vibration where the first damper 11 mainly acts, and when the large amplitude of vibration beyond the practical amplitude of vibration is applied, the second damper 12 is gradually effected to apply a suitable braking on the large amplitude of vibration, and thus high input resistance can be obtained. Further, the torsional rigidity of the damper 10 for a speaker is improved by the annular space S that is formed as a part of the first damper 11 and the second damper 12, whereby the vibration of the voice coil 30 can be suitably regulated in one axis direction against the rolling of the voice coil 30 and so forth. Thus, the sound quality can be improved compared to an input resistance speaker at the same level by improving the linearity, and the reliability can be improved compared to a high compliance speaker at the same level by restraining the damage and the rolling when large amplitude of vibration is inputted.
Further, in the damper 10 for a speaker, both the outer periphery part 11b of the first damper 11 and the outer periphery part 12b of the second damper 12 that are coupled to the voice coil 30 or the voice coil support part 31 are coupled to the frame 2, whereby even if a peel-off occurs at the coupling surface of either one of the first damper 11 and the second damper 12, the supporting force for the voice coil 30 can be maintained by the damper 10 for a speaker, thereby preventing the speaker device 1 from being damaged.
In the speaker device 1 shown in
In the example shown in
As such, the damper 10 for a speaker can be formed with a plurality of damper members. As shown in this example, by adding the third damper 15, more variations are available for adjusting the action of the damper 10 for a speaker when large amplitude of vibration is applies. Further, arbitrary adjustment is available in response to a request for symmetricity or asymmetricity of the vertical vibration of the voice coil 30. In the example of the drawing, the first damper 11, the second damper 12 and the third damper 15 have cross-sectional shapes different from each other. Each cross-sectional shape is arbitrarily determined in response to a request for the symmetricity or the asymmetricity of the vertical vibration of the voice coil 30 and so on. Further, the curved top part of the first damper, the virtual curved top part of the second damper, and the curved top part of the third damper may be provided at the positions different from each other, or they may be provided at the positions in the proximity of each other or substantially at the same positions.
The example shown in
In the example shown in
If a plurality of dampers 10 for a speaker are provided as described above, a holding force of the voice coil 30 can be strengthened, a rolling is restrained (vibration direction is more strongly controlled), braking performance is strengthened against the large amplitude of vibration being applied, a force applied to the damper 10 for a speaker in the manufacturing process is shared by a plurality of dampers, and the damper 10 for a speaker can be arranged at a given position. In the example shown in the drawing, the dampers 10X, 10Y for a speaker are attached to the frame side via a space member 17 as another member by attaching to the frame side at one time the space member 17 and the dampers 10X, 10Y for a speaker which are preliminarily attached the space member 17.
In the example shown in
In the aforementioned embodiments except the example shown in
As describe above, the damper 10 for a speaker and the speaker device 1 according to an embodiment of the present invention can operate with both a high compliance and a low compliance and can achieve a high sound quality with a high linearity within the practical amplitude of vibration while producing loud sound. Such a speaker device can be used as a variety of electronic devices and in-car devices.
Further, when the speaker device 1 is mounted on the wall or ceiling as an attaching counterpart in buildings including a residential house (building) or a hotel, an inn, training facilities and so force (building), which can accommodate many guests for conferences, meetings, lectures, parties and so on, the speaker device 1 can produce loud sound with a high sound quality, and thereby enabling the achievement of residential space equipped with high-quality audiovisual facility.
The embodiments according to the present invention are described in detail with reference to the drawings, however specific configurations are not limited to these embodiments and any design alterations without departing from the scope of the present invention are included in the present invention. Further, the technologies of each embodiment as described above can be used by each other, unless specific contradictions or problems are involved in their objects, the configurations, and so forth.
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/JP2009/061883 | 6/29/2009 | WO | 00 | 12/28/2011 |