BONE CONDUCTION SPEAKER AND COMPOUND VIBRATION DEVICE THEREOF

Abstract

The present invention relates to a bone conduction speaker and its compound vibration device. The compound vibration device comprises a vibration conductive plate and a vibration board, the vibration conductive plate is set to be the first torus, where at least two first rods inside it converge to its center; the vibration board is set as the second torus, where at least two second rods inside it converge to its center. The vibration conductive plate is fixed with the vibration board; the first torus is fixed on a magnetic system, and the second torus comprises a fixed voice coil, which is driven by the magnetic system. The bone conduction speaker in the present invention and its compound vibration device adopt the fixed vibration conductive plate and vibration board, making the technique simpler with a lower cost; because the two adjustable parts in the compound vibration device can adjust both low frequency and high frequency area, the frequency response obtained is flatter and the sound is broader.

Claims

1. A vibration device, comprising: a housing; compound vibration parts residing inside the housing and connected to a magnet component, wherein the compound vibration parts include two or more vibration parts at least partially attached to each other, at least two of the two or more vibration parts having different stiffness coefficients, the magnet component is configured to drive a voice coil to vibrate, the vibration of the voice coil drives the compound vibration parts to generate vibrations, the vibrations of the compound vibration parts produce a sound wave inside the housing and cause a leaked sound wave spreading outside the housing, and the housing includes a contact surface to contact a user, the contact surface including one or more holes, the one or more holes being configured to guide the sound wave inside the housing through the one or more holes to an outside of the housing, the guided sound wave interfering with the leaked sound wave.

2. The vibration device according to claim 1, wherein the two or more vibration parts include a first torus and a second torus, a radius of the first torus is smaller than a radius of the second torus.

3. The vibration device according to claim 1, wherein the two or more vibration parts overlap each other.

4. The vibration device according to claim 1, wherein at least part of the compound vibration parts is connected to the housing.

5. The vibration device according to claim 1, wherein at least one of the two or more vibration parts is an elastic plate.

6. The vibration device according to claim 1, wherein a thickness of at least one of the two or more vibration parts is in a range of 0.005 mm-3 mm.

7. The vibration device according to claim 6, wherein a thickness of at least one of the two or more vibration parts is in a range of 0.02 mm-0.5 mm.

8. The vibration device according to claim 1, wherein a hollow pattern is disposed on at least one of the two or more vibration parts.

9. The vibration device according to claim 8, wherein an area of the hollow pattern is not less than an area of non-hollow portion on the at least one of the two or more vibration parts.

10. The vibration device according to claim 1, wherein at least one of the two or more vibration parts has a different thickness distribution.

11. The vibration device according to claim 1, wherein at least part of the compound vibration parts is fixed on the magnetic component via a grommet.

12. The vibration device according to claim 1, wherein the voice coil is fixed on at least part of the compound vibration parts.

13. The vibration device according to claim 1, wherein the magnetic component comprises: a bottom plate; an annular magnet attaching to the bottom plate; an inner magnet concentrically disposed inside the annular magnet; an inner magnetic conductive plate attaching to the inner magnet; an annular magnetic conductive plate attaching to the annular magnet; and a grommet attaching to the annular magnetic conductive plate.

14. A speaker, comprising a vibration device including: a housing; compound vibration parts residing inside the housing and connected to a magnet component, wherein the compound vibration parts include two or more vibration parts at least partially attached to each other, at least two of the two or more vibration parts having different stiffness coefficients, the magnet component is configured to drive a voice coil to vibrate, the vibration of the voice coil drives the compound vibration parts to generate vibrations, the vibrations of the compound vibration parts produce a sound wave inside the housing and cause a leaked sound wave spreading outside the housing, and the housing includes a contact surface to contact a user, the contact surface including one or more holes, the one or more holes being configured to guide the sound wave inside the housing through the one or more holes to an outside of the housing, the guided sound wave interfering with the leaked sound wave.

15. The speaker according to claim 14, wherein the two or more vibration parts include a first torus and a second torus, a radius of the first torus is smaller than a radius of the second torus.

16. The speaker according to claim 14, wherein the two or more vibration parts overlap each other.

17. The speaker according to claim 14, wherein at least part of the compound vibration parts is connected to the housing.

18. The speaker according to claim 14, wherein at least one of the two or more vibration parts is an elastic plate.

19. The speaker according to claim 14, wherein a thickness of at least one of the two or more vibration parts is in a range of 0.005 mm-3 mm.

20. The speaker according to claim 14, wherein at least one of the two or more vibration parts has a different thickness distribution.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0019] FIG. 1: Longitudinal section view of the bone conduction speaker in the present invention;

[0020] FIG. 2: Perspective view of the vibration parts in the bone conduction speaker in the present invention;

[0021] FIG. 3: Exploded perspective view of the bone conduction speaker in the present invention;

[0022] FIG. 4: Frequency response curves of the bone conduction speakers of vibration device in the prior art;

[0023] FIG. 5: Frequency response curves of the bone conduction speakers of the vibration device in the present invention;

[0024] FIG. 6: Perspective view of the bone conduction speaker in the present invention;

[0025] FIG. 7 illustrates a structure of the bone conduction speaker and the compound vibration device according to some embodiments of the present disclosure;

[0026] FIG. 8-A illustrates an equivalent vibration model of the vibration portion of the bone conduction speaker according to some embodiments of the present disclosure;

[0027] FIG. 8-B illustrates a vibration response curve of the bone conduction speaker according to one specific embodiment of the present disclosure;

[0028] FIG. 8-C illustrates a vibration response curve of the bone conduction speaker according to one specific embodiment of the present disclosure;

[0029] FIG. 9-A illustrates a structure of the vibration generation portion of the bone conduction speaker according to one specific embodiment of the present disclosure;

[0030] FIG. 9-B illustrates a vibration response curve of the bone conduction speaker according to one specific embodiment of the present disclosure;

[0031] FIG. 9-C illustrates a sound leakage curve of the bone conduction speaker according to one specific embodiment of the present disclosure;

[0032] FIG. 10 illustrates a structure of the vibration generation portion of the bone conduction speaker according to one specific embodiment of the present disclosure;

[0033] FIG. 11-A illustrates an application scenario of the bone conduction speaker according to one specific embodiment of the present disclosure;

[0034] FIG. 11-B illustrates a vibration response curve of the bone conduction speaker according to one specific embodiment of the present disclosure;

[0035] FIG. 12 illustrates a structure of the vibration generation portion of the bone conduction speaker according to one specific embodiment of the present disclosure; and

[0036] FIG. 13 illustrates a structure of the vibration generation portion of the bone conduction speaker according to one specific embodiment of the present disclosure.

DETAILED DESCRIPTION

[0037] A detailed description of the implements of the present invention is stated here, together with attached figures.

[0038] As shown in FIG. 1 and FIG. 3, the compound vibration device in the present invention of bone conduction speaker, comprises: the compound vibration parts composed of vibration conductive plate 1 and vibration board 2, the vibration conductive plate 1 is set as the first torus 111 and three first rods 112 in the first torus converging to the center of the torus, the converging center is fixed with the center of the vibration board 2. The center of the vibration board 2 is an indentation 120, which matches the converging center and the first rods. The vibration board 2 contains a second torus 121, which has a smaller radius than the vibration conductive plate 1, as well as three second rods 122, which is thicker and wider than the first rods 112. The first rods 112 and the second rods 122 are staggered, present but not limited to an angle of 60 degrees, as shown in FIG. 2. A better solution is, both the first and second rods are all straight rods.

[0039] Obviously the number of the first and second rods can be more than two, for example, if there are two rods, they can be set in a symmetrical position; however, the most economic design is working with three rods. Not limited to this rods setting mode, the setting of rods in the present invention can also be a spoke structure with four, five or more rods.

[0040] The vibration conductive plate 1 is very thin and can be more elastic, which is stuck at the center of the indentation 120 of the vibration board 2. Below the second torus 121 spliced in vibration board 2 is a voice coil 8. The compound vibration device in the present invention also comprises a bottom plate 12, where an annular magnet 10 is set, and an inner magnet 11 is set in the annular magnet 10 concentrically. An inner magnet conduction plate 9 is set on the top of the inner magnet 11, while annular magnet conduction plate 7 is set on the annular magnet 10, a grommet 6 is fixed above the annular magnet conduction plate 7, the first torus 111 of the vibration conductive plate 1 is fixed with the grommet 6. The whole compound vibration device is connected to the outside through a panel 13, the panel 13 is fixed with the vibration conductive plate 1 on its converging center, stuck and fixed at the center of both vibration conductive plate 1 and vibration board 2.

[0041] It should be noted that, both the vibration conductive plate and the vibration board can be set more than one, fixed with each other through either the center or staggered with both center and edge, forming a multilayer vibration structure, corresponding to different frequency resonance ranges, thus achieve a high tone quality earphone vibration unit with a gamut and full frequency range, despite of the higher cost.

[0042] The bone conduction speaker contains a magnet system, composed of the annular magnet conductive plate 7, annular magnet 10, bottom plate 12, inner magnet 11 and inner magnet conductive plate 9, because the changes of audio-frequency current in the voice coil 8 cause changes of magnet field, which makes the voice coil 8 vibrate. The compound vibration device is connected to the magnet system through grommet 6. The bone conduction speaker connects with the outside through the panel 13, being able to transfer vibrations to human bones.

[0043] In the better implement examples of the present bone conduction speaker and its compound vibration device, the magnet system, composed of the annular magnet conductive plate 7, annular magnet 10, inner magnet conduction plate 9, inner magnet 11 and bottom plate 12, interacts with the voice coil which generates changing magnet field intensity when its current is changing, and inductance changes accordingly, forces the voice coil 8 move longitudinally, then causes the vibration board 2 to vibrate, transfers the vibration to the vibration conductive plate 1, then, through the contact between panel 13 and the post ear, cheeks or forehead of the human beings, transfers the vibrations to human bones, thus generates sounds. A complete product unit is shown in FIG. 6.

[0044] Through the compound vibration device composed of the vibration board and the vibration conductive plate, a frequency response shown in FIG. 5 is achieved. The double compound vibration generates two resonance peaks, whose positions can be changed by adjusting the parameters including sizes and materials of the two vibration parts, making the resonance peak in low frequency area move to the lower frequency area and the peak in high frequency move higher, finally generates a frequency response curve as the dotted line shown in FIG. 5, which is a flat frequency response curve generated in an ideal condition, whose resonance peaks are among the frequencies catchable with human ears. Thus, the device widens the resonance oscillation ranges, and generates the ideal voices.

[0045] In some embodiments, the stiffness of the vibration board may be larger than that of the vibration conductive plate. In some embodiments, the resonance peaks of the frequency response curve may be set within a frequency range perceivable by human ears, or a frequency range that a person's ears may not hear. Preferably, the two resonance peaks may be beyond the frequency range that a person may hear. More preferably, one resonance peak may be within the frequency range perceivable by human ears, and another one may be beyond the frequency range that a person may hear. More preferably, the two resonance peaks may be within the frequency range perceivable by human ears. Further preferably, the two resonance peaks may be within the frequency range perceivable by human ears, and the peak frequency may be in a range of 80 Hz-18000 Hz. Further preferably, the two resonance peaks may be within the frequency range perceivable by human ears, and the peak frequency may be in a range of 200 Hz-15000 Hz. Further preferably, the two resonance peaks may be within the frequency range perceivable by human ears, and the peak frequency may be in a range of 500 Hz-12000 Hz. Further preferably, the two resonance peaks may be within the frequency range perceivable by human ears, and the peak frequency may be in a range of 800 Hz-11000 Hz. There may be a difference between the frequency values of the resonance peaks. For example, the difference between the frequency values of the two resonance peaks may be at least 500 Hz, preferably 1000 Hz, more preferably 2000 Hz, and more preferably 5000 Hz. To achieve a better effect, the two resonance peaks may be within the frequency range perceivable by human ears, and the difference between the frequency values of the two resonance peaks may be at least 500 Hz. Preferably, the two resonance peaks may be within the frequency range perceivable by human ears, and the difference between the frequency values of the two resonance peaks may be at least 1000 Hz. More preferably, the two resonance peaks may be within the frequency range perceivable by human ears, and the difference between the frequency values of the two resonance peaks may be at least 2000 Hz. More preferably, the two resonance peaks may be within the frequency range perceivable by human ears, and the difference between the frequency values of the two resonance peaks may be at least 3000 Hz. Moreover, more preferably, the two resonance peaks may be within the frequency range perceivable by human ears, and the difference between the frequency values of the two resonance peaks may be at least 4000 Hz. One resonance peak may be within the frequency range perceivable by human ears, another one may be beyond the frequency range that a person may hear, and the difference between the frequency values of the two resonance peaks may be at least 500 Hz. Preferably, one resonance peak may be within the frequency range perceivable by human ears, another one may be beyond the frequency range that a person may hear, and the difference between the frequency values of the two resonance peaks may be at least 1000 Hz. More preferably, one resonance peak may be within the frequency range perceivable by human ears, another one may be beyond the frequency range that a person may hear, and the difference between the frequency values of the two resonance peaks may be at least 2000 Hz. More preferably, one resonance peak may be within the frequency range perceivable by human ears, another one may be beyond the frequency range that a person may hear, and the difference between the frequency values of the two resonance peaks may be at least 3000 Hz. Moreover, more preferably, one resonance peak may be within the frequency range perceivable by human ears, another one may be beyond the frequency range that a person may hear, and the difference between the frequency values of the two resonance peaks may be at least 4000 Hz. Both resonance peaks may be within the frequency range of 5 Hz-30000 Hz, and the difference between the frequency values of the two resonance peaks may be at least 400 Hz. Preferably, both resonance peaks may be within the frequency range of 5 Hz-30000 Hz, and the difference between the frequency values of the two resonance peaks may be at least 1000 Hz. More preferably, both resonance peaks may be within the frequency range of 5 Hz-30000 Hz, and the difference between the frequency values of the two resonance peaks may be at least 2000 Hz. More preferably, both resonance peaks may be within the frequency range of 5 Hz-30000 Hz, and the difference between the frequency values of the two resonance peaks may be at least 3000 Hz. Moreover, further preferably, both resonance peaks may be within the frequency range of 5 Hz-30000 Hz, and the difference between the frequency values of the two resonance peaks may be at least 4000 Hz. Both resonance peaks may be within the frequency range of 20 Hz-20000 Hz, and the difference between the frequency values of the two resonance peaks may be at least 400 Hz. Preferably, both resonance peaks may be within the frequency range of 20 Hz-20000 Hz, and the difference between the frequency values of the two resonance peaks may be at least 1000 Hz. More preferably, both resonance peaks may be within the frequency range of 20 Hz-20000 Hz, and the difference between the frequency values of the two resonance peaks may be at least 2000 Hz. More preferably, both resonance peaks may be within the frequency range of 20 Hz-20000 Hz, and the difference between the frequency values of the two resonance peaks may be at least 3000 Hz. And further preferably, both resonance peaks may be within the frequency range of 20 Hz-20000 Hz, and the difference between the frequency values of the two resonance peaks may be at least 4000 Hz. Both the two resonance peaks may be within the frequency range of 100 Hz-18000 Hz, and the difference between the frequency values of the two resonance peaks may be at least 400 Hz. Preferably, both resonance peaks may be within the frequency range of 100 Hz-18000 Hz, and the difference between the frequency values of the two resonance peaks may be at least 1000 Hz. More preferably, both resonance peaks may be within the frequency range of 100 Hz-18000 Hz, and the difference between the frequency values of the two resonance peaks may be at least 2000 Hz. More preferably, both resonance peaks may be within the frequency range of 100 Hz-18000 Hz, and the difference between the frequency values of the two resonance peaks may be at least 3000 Hz. And further preferably, both resonance peaks may be within the frequency range of 100 Hz-18000 Hz, and the difference between the frequency values of the two resonance peaks may be at least 4000 Hz. Both the two resonance peaks may be within the frequency range of 200 Hz-12000 Hz, and the difference between the frequency values of the two resonance peaks may be at least 400 Hz. Preferably, both resonance peaks may be within the frequency range of 200 Hz-12000 Hz, and the difference between the frequency values of the two resonance peaks may be at least 1000 Hz. More preferably, both resonance peaks may be within the frequency range of 200 Hz-12000 Hz, and the difference between the frequency values of the two resonance peaks may be at least 2000 Hz. More preferably, both resonance peaks may be within the frequency range of 200 Hz-12000 Hz, and the difference between the frequency values of the two resonance peaks may be at least 3000 Hz. And further preferably, both resonance peaks may be within the frequency range of 200 Hz-12000 Hz, and the difference between the frequency values of the two resonance peaks may be at least 4000 Hz. Both the two resonance peaks may be within the frequency range of 500 Hz-10000 Hz, and the difference between the frequency values of the two resonance peaks may be at least 400 Hz. Preferably, both resonance peaks may be within the frequency range of 500 Hz-10000 Hz, and the difference between the frequency values of the two resonance peaks may be at least 1000 Hz. More preferably, both resonance peaks may be within the frequency range of 500 Hz-10000 Hz, and the difference between the frequency values of the two resonance peaks may be at least 2000 Hz. More preferably, both resonance peaks may be within the frequency range of 500 Hz-10000 Hz, and the difference between the frequency values of the two resonance peaks may be at least 3000 Hz. And further preferably, both resonance peaks may be within the frequency range of 500 Hz-10000 Hz, and the difference between the frequency values of the two resonance peaks may be at least 4000 Hz. This may broaden the range of the resonance response of the speaker, thus obtaining a more ideal sound quality. It should be noted that in actual applications, there may be multiple vibration conductive plates and vibration boards to form multi-layer vibration structures corresponding to different ranges of frequency response, thus obtaining diatonic, full-ranged and high-quality vibrations of the speaker, or may make the frequency response curve meet requirements in a specific frequency range. For example, to satisfy the requirement of normal hearing, a bone conduction hearing aid may be configured to have a transducer including one or more vibration boards and vibration conductive plates with a resonance frequency in a range of 100 Hz-10000 Hz.

[0046] In the better implement examples, but, not limited to these examples, it is adopted that, the vibration conductive plate can be made by stainless steels, with a thickness of 0.1-0.2 mm, and when the middle three rods of the first rods group in the vibration conductive plate have a width of 0.5-1.0 mm, the low frequency resonance oscillation peak of the bone conduction speaker is located between 300 and 900 Hz. And, when the three straight rods in the second rods group have a width between 1.6 and 2.6 mm, and a thickness between 0.8 and 1.2 mm, the high frequency resonance oscillation peak of the bone conduction speaker is between 7500 and 9500 Hz. Also, the structures of the vibration conductive plate and the vibration board is not limited to three straight rods, as long as their structures can make a suitable flexibility to both vibration conductive plate and vibration board, cross-shaped rods and other rod structures are also suitable. Of course, with more compound vibration parts, more resonance oscillation peaks will be achieved, and the fitting curve will be flatter and the sound wider. Thus, in the better implement examples, more than two vibration parts, including the vibration conductive plate and vibration board as well as similar parts, overlapping each other, is also applicable, just needs more costs.

[0047] As shown in FIG. 7, in another embodiment, the compound vibration device (also referred to as “compound vibration system”) may include a vibration board 702, a first vibration conductive plate 703, and a second vibration conductive plate 701. The first vibration conductive plate 703 may fix the vibration board 702 and the second vibration conductive plate 701 onto a housing 719. The compound vibration system including the vibration board 702, the first vibration conductive plate 703, and the second vibration conductive plate 701 may lead to no less than two resonance peaks and a smoother frequency response curve in the range of the auditory system, thus improving the sound quality of the bone conduction speaker. The equivalent model of the compound vibration system may be shown in FIG. 8-A:

[0048] For illustration purposes, 801 represents a housing, 802 represents a panel, 803 represents a voice coil, 804 represents a magnetic circuit system, 805 represents a first vibration conductive plate, 806 represents a second vibration conductive plate, and 807 represents a vibration board. The first vibration conductive plate, the second vibration conductive plate, and the vibration board may be abstracted as components with elasticity and damping; the housing, the panel, the voice coil and the magnetic circuit system may be abstracted as equivalent mass blocks. The vibration equation of the system may be expressed as:

m.sub.6x.sub.6″R.sub.6(x.sub.6−x.sub.5)′+k.sub.6(x.sub.6−x.sub.5)=F,  (1)

x.sub.7θ+R.sub.7(x.sub.7−x.sub.5)′+k.sub.7(x.sub.7−x.sub.5)=−F,  (2)

m.sub.5x.sub.5″−R.sub.6(x.sub.6−x.sub.5)′−R.sub.7(x.sub.7−x.sub.5)′R.sub.8x.sub.5′+k.sub.8x.sub.5−k.sub.6(x.sub.6−x.sub.5)−k.sub.7(x.sub.7−x.sub.5)=0,  (3)

wherein, F is a driving force, k.sub.6 is an equivalent stiffness coefficient of the second vibration conductive plate, k.sub.7 is an equivalent stiffness coefficient of the vibration board, k.sub.8 is an equivalent stiffness coefficient of the first vibration conductive plate, R.sub.6 is an equivalent damping of the second vibration conductive plate, R.sub.7 is an equivalent damping of the vibration board, R.sub.8 is an equivalent damp of the first vibration conductive plate, m.sub.5 is a mass of the panel, m.sub.6 is a mass of the magnetic circuit system, m.sub.7 is a mass of the voice coil, x.sub.5 is a displacement of the panel, x.sub.6 is a displacement of the magnetic circuit system, x.sub.7 is to displacement of the voice coil, and the amplitude of the panel 802 may be:

[00001]$\begin{array}{cc}{A}_5=\frac{\left(-m_6{\omega }^2\left({\mathrm{jR}}_7\omega -k_7\right)+m_7{\omega }^2\left({\mathrm{jR}}_6\omega -k_6\right)\right)}{\left(\begin{array}{c}\left(-m_5{\omega }^2-{\mathrm{jR}}_8\omega +k_8\right)\left(-m_6{\omega }^2-{\mathrm{jR}}_6\omega +k_6\right)(-m_7{\omega }^2-\\ {\mathrm{jR}}_7\omega +k_7)-m_6{\omega }^2\left(-{\mathrm{jR}}_6\omega +k_6\right)\left(-m_7{\omega }^2-{\mathrm{jR}}_7\omega +k_7\right)-\\ m_7{\omega }^2\left(-{\mathrm{jR}}_7\omega +k_7\right)\left(-m_6{\omega }^2-{\mathrm{jR}}_6\omega +k_6\right)\end{array}\right)}{f}_0,& \left(4\right)\end{array}$

wherein ω is an angular frequency of the vibration, and f.sub.0 is a unit driving force.

[0049] The vibration system of the bone conduction speaker may transfer vibrations to a user via a panel (e.g., the panel 730 shown in FIG. 7). According to the equation (4), the vibration efficiency may relate to the stiffness coefficients of the vibration board, the first vibration conductive plate, and the second vibration conductive plate, and the vibration damping. Preferably, the stiffness coefficient of the vibration board k.sub.7 may be greater than the second vibration coefficient k.sub.6, and the stiffness coefficient of the vibration board k.sub.7 may be greater than the first vibration factor k.sub.8. The number of resonance peaks generated by the compound vibration system with the first vibration conductive plate may be more than the compound vibration system without the first vibration conductive plate, preferably at least three resonance peaks. More preferably, at least one resonance peak may be beyond the range perceivable by human ears. More preferably, the resonance peaks may be within the range perceivable by human ears. More further preferably, the resonance peaks may be within the range perceivable by human ears, and the frequency peak value may be no more than 18000 Hz. More preferably, the resonance peaks may be within the range perceivable by human ears, and the frequency peak value may be within the frequency range of 100 Hz-15000 Hz. More preferably, the resonance peaks may be within the range perceivable by human ears, and the frequency peak value may be within the frequency range of 200 Hz-12000 Hz. More preferably, the resonance peaks may be within the range perceivable by human ears, and the frequency peak value may be within the frequency range of 500 Hz-11000 Hz. There may be differences between the frequency values of the resonance peaks. For example, there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks no less than 200 Hz. Preferably, there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks no less than 500 Hz. More preferably, there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks no less than 1000 Hz. More preferably, there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks no less than 2000 Hz. More preferably, there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks no less than 5000 Hz. To achieve a better effect, all of the resonance peaks may be within the range perceivable by human ears, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks no less than 500 Hz. Preferably, all of the resonance peaks may be within the range perceivable by human ears, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks no less than 1000 Hz. More preferably, all of the resonance peaks may be within the range perceivable by human ears, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks no less than 2000 Hz. More preferably, all of the resonance peaks may be within the range perceivable by human ears, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks no less than 3000 Hz. More preferably, all of the resonance peaks may be within the range perceivable by human ears, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks no less than 4000 Hz. Two of the three resonance peaks may be within the frequency range perceivable by human ears, and another one may be beyond the frequency range that a person may hear, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks no less than 500 Hz. Preferably, two of the three resonance peaks may be within the frequency range perceivable by human ears, and another one may be beyond the frequency range that a person may hear, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks no less than 1000 Hz. More preferably, two of the three resonance peaks may be within the frequency range perceivable by human ears, and another one may be beyond the frequency range that a person may hear, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks no less than 2000 Hz. More preferably, two of the three resonance peaks may be within the frequency range perceivable by human ears, and another one may be beyond the frequency range that a person may hear, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks no less than 3000 Hz. More preferably, two of the three resonance peaks may be within the frequency range perceivable by human ears, and another one may be beyond the frequency range that a person may hear, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks no less than 4000 Hz. One of the three resonance peaks may be within the frequency range perceivable by human ears, and the other two may be beyond the frequency range that a person may hear, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks no less than 500 Hz. Preferably, one of the three resonance peaks may be within the frequency range perceivable by human ears, and the other two may be beyond the frequency range that a person may hear, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks no less than 1000 Hz. More preferably, one of the three resonance peaks may be within the frequency range perceivable by human ears, and the other two may be beyond the frequency range that a person may hear, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks no less than 2000 Hz. More preferably, one of the three resonance peaks may be within the frequency range perceivable by human ears, and the other two may be beyond the frequency range that a person may hear, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks no less than 3000 Hz. More preferably, one of the three resonance peaks may be within the frequency range perceivable by human ears, and the other two may be beyond the frequency range that a person may hear, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks no less than 4000 Hz. All the resonance peaks may be within the frequency range of 5 Hz-30000 Hz, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks of at least 400 Hz. Preferably, all the resonance peaks may be within the frequency range of 5 Hz-30000 Hz, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks of at least 1000 Hz. More preferably, all the resonance peaks may be within the frequency range of 5 Hz-30000 Hz, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks of at least 2000 Hz. More preferably, all the resonance peaks may be within the frequency range of 5 Hz-30000 Hz, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks of at least 3000 Hz. And further preferably, all the resonance peaks may be within the frequency range of 5 Hz-30000 Hz, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks of at least 4000 Hz. All the resonance peaks may be within the frequency range of 20 Hz-20000 Hz, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks of at least 400 Hz. Preferably, all the resonance peaks may be within the frequency range of 20 Hz-20000 Hz, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks of at least 1000 Hz. More preferably, all the resonance peaks may be within the frequency range of 20 Hz-20000 Hz, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks of at least 2000 Hz. More preferably, all the resonance peaks may be within the frequency range of 20 Hz-20000 Hz, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks of at least 3000 Hz. And further preferably, all the resonance peaks may be within the frequency range of 20 Hz-20000 Hz, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks of at least 4000 Hz. All the resonance peaks may be within the frequency range of 100 Hz-18000 Hz, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks of at least 400 Hz. Preferably, all the resonance peaks may be within the frequency range of 100 Hz-18000 Hz, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks of at least 1000 Hz. More preferably, all the resonance peaks may be within the frequency range of 100 Hz-18000 Hz, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks of at least 2000 Hz. More preferably, all the resonance peaks may be within the frequency range of 100 Hz-18000 Hz, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks of at least 3000 Hz. And further preferably, all the resonance peaks may be within the frequency range of 100 Hz-18000 Hz, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks of at least 4000 Hz. All the resonance peaks may be within the frequency range of 200 Hz-12000 Hz, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks of at least 400 Hz. Preferably, all the resonance peaks may be within the frequency range of 200 Hz-12000 Hz, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks of at least 1000 Hz. More preferably, all the resonance peaks may be within the frequency range of 200 Hz-12000 Hz, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks of at least 2000 Hz. More preferably, all the resonance peaks may be within the frequency range of 200 Hz-12000 Hz, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks of at least 3000 Hz. And further preferably, all the resonance peaks may be within the frequency range of 200 Hz-12000 Hz, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks of at least 4000 Hz. All the resonance peaks may be within the frequency range of 500 Hz-10000 Hz, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks of at least 400 Hz. Preferably, all the resonance peaks may be within the frequency range of 500 Hz-10000 Hz, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks of at least 1000 Hz. More preferably, all the resonance peaks may be within the frequency range of 500 Hz-10000 Hz, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks of at least 2000 Hz. More preferably, all the resonance peaks may be within the frequency range of 500 Hz-10000 Hz, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks of at least 3000 Hz. Moreover, further preferably, all the resonance peaks may be within the frequency range of 500 Hz-10000 Hz, and there may be at least two resonance peaks with a difference of the frequency values between the two resonance peaks of at least 4000 Hz. In one embodiment, the compound vibration system including the vibration board, the first vibration conductive plate, and the second vibration conductive plate may generate a frequency response as shown in FIG. 8-B. The compound vibration system with the first vibration conductive plate may generate three obvious resonance peaks, which may improve the sensitivity of the frequency response in the low-frequency range (about 600 Hz), obtain a smoother frequency response, and improve the sound quality.

[0050] The resonance peak may be shifted by changing a parameter of the first vibration conductive plate, such as the size and material, so as to obtain an ideal frequency response eventually. For example, the stiffness coefficient of the first vibration conductive plate may be reduced to a designed value, causing the resonance peak to move to a designed low frequency, thus enhancing the sensitivity of the bone conduction speaker in the low frequency, and improving the quality of the sound. As shown in FIG. 8-C, as the stiffness coefficient of the first vibration conductive plate decreases (i.e., the first vibration conductive plate becomes softer), the resonance peak moves to the low frequency region, and the sensitivity of the frequency response of the bone conduction speaker in the low frequency region gets improved. Preferably, the first vibration conductive plate may be an elastic plate, and the elasticity may be determined based on the material, thickness, structure, or the like. The material of the first vibration conductive plate may include but not limited to steel (for example but not limited to, stainless steel, carbon steel, etc.), light alloy (for example but not limited to, aluminum, beryllium copper, magnesium alloy, titanium alloy, etc.), plastic (for example but not limited to, polyethylene, nylon blow molding, plastic, etc.). It may be a single material or a composite material that achieve the same performance. The composite material may include but not limited to reinforced material, such as glass fiber, carbon fiber, boron fiber, graphite fiber, graphene fiber, silicon carbide fiber, aramid fiber, or the like. The composite material may also be other organic and/or inorganic composite materials, such as various types of glass fiber reinforced by unsaturated polyester and epoxy, fiberglass comprising phenolic resin matrix. The thickness of the first vibration conductive plate may be not less than 0.005 mm. Preferably, the thickness may be 0.005 mm-3 mm. More preferably, the thickness may be 0.01 mm-2 mm. More preferably, the thickness may be 0.01 mm-1 mm. Moreover, further preferably, the thickness may be 0.02 mm-0.5 mm. The first vibration conductive plate may have an annular structure, preferably including at least one annular ring, preferably, including at least two annular rings. The annular ring may be a concentric ring or a non-concentric ring and may be connected to each other via at least two rods converging from the outer ring to the center of the inner ring. More preferably, there may be at least one oval ring. More preferably, there may be at least two oval rings. Different oval rings may have different curvatures radiuses, and the oval rings may be connected to each other via rods. Further preferably, there may be at least one square ring. The first vibration conductive plate may also have the shape of a plate. Preferably, a hollow pattern may be configured on the plate. Moreover, more preferably, the area of the hollow pattern may be not less than the area of the non-hollow portion. It should be noted that the above-described material, structure, or thickness may be combined in any manner to obtain different vibration conductive plates. For example, the annular vibration conductive plate may have a different thickness distribution. Preferably, the thickness of the ring may be equal to the thickness of the rod. Further preferably, the thickness of the rod may be larger than the thickness of the ring. Moreover, still, further preferably, the thickness of the inner ring may be larger than the thickness of the outer ring.

[0051] When the compound vibration device is applied to the bone conduction speaker, the major applicable area is bone conduction earphones. Thus the bone conduction speaker adopting the structure will be fallen into the protection of the present invention.

[0052] The bone conduction speaker and its compound vibration device stated in the present invention, make the technique simpler with a lower cost. Because the two parts in the compound vibration device can adjust the low frequency as well as the high frequency ranges, as shown in FIG. 5, which makes the achieved frequency response flatter, and voice more broader, avoiding the problem of abrupt frequency response and feeble voices caused by single vibration device, thus broaden the application prospection of bone conduction speaker.

[0053] In the prior art, the vibration parts did not take full account of the effects of every part to the frequency response, thus, although they could have the similar outlooks with the products described in the present invention, they will generate an abrupt frequency response, or feeble sound. And due to the improper matching between different parts, the resonance peak could have exceeded the human hearable range, which is between 20 Hz and 20 KHz. Thus, only one sharp resonance peak as shown in FIG. 4 appears, which means a pretty poor tone quality.

[0054] It should be made clear that, the above detailed description of the better implement examples should not be considered as the limitations to the present invention protections. The extent of the patent protection of the present invention should be determined by the terms of claims.

EXAMPLES

Example 1

[0055] A bone conduction speaker may include a U-shaped headset bracket/headset lanyard, two vibration units, a transducer connected to each vibration unit. The vibration unit may include a contact surface and a housing. The contact surface may be an outer surface of a silicone rubber transfer layer and may be configured to have a gradient structure including a convex portion. A clamping force between the contact surface and skin due to the headset bracket/headset lanyard may be unevenly distributed on the contact surface. The sound transfer efficiency of the portion of the gradient structure may be different from the portion without the gradient structure.

Example 2

[0056] This example may be different from Example 1 in the following aspects. The headset bracket/headset lanyard as described may include a memory alloy. The headset bracket/headset lanyard may match the curves of different users' heads and have a good elasticity and a better wearing comfort. The headset bracket/headset lanyard may recover to its original shape from a deformed status last for a certain period. As used herein, the certain period may refer to ten minutes, thirty minutes, one hour, two hours, five hours, or may also refer to one day, two days, ten days, one month, one year, or a longer period. The clamping force that the headset bracket/headset lanyard provides may keep stable, and may not decline gradually over time. The force intensity between the bone conduction speaker and the body surface of a user may be within an appropriate range, so as to avoid pain or clear vibration sense caused by undue force when the user wears the bone conduction speaker. Moreover, the clamping force of bone conduction speaker may be within a range of 0.2N˜1.5N when the bone conduction speaker is used.

Example 3

[0057] The difference between this example and the two examples mentioned above may include the following aspects. The elastic coefficient of the headset bracket/headset lanyard may be kept in a specific range, which results in the value of the frequency response curve in low frequency (e.g., under 500 Hz) being higher than the value of the frequency response curve in high frequency (e.g., above 4000 Hz).

Example 4

[0058] The difference between Example 4 and Example 1 may include the following aspects. The bone conduction speaker may be mounted on an eyeglass frame, or in a helmet or mask with a special function.

Example 5

[0059] The difference between this example and Example 1 may include the following aspects. The vibration unit may include two or more panels, and the different panels or the vibration transfer layers connected to the different panels may have different gradient structures on a contact surface being in contact with a user. For example, one contact surface may have a convex portion, the other one may have a concave structure, or the gradient structures on both the two contact surfaces may be convex portions or concave structures, but there may be at least one difference between the shape or the number of the convex portions.

Example 6

[0060] A portable bone conduction hearing aid may include multiple frequency response curves. A user or a tester may choose a proper response curve for hearing compensation according to an actual response curve of the auditory system of a person. In addition, according to an actual requirement, a vibration unit in the bone conduction hearing aid may enable the bone conduction hearing aid to generate an ideal frequency response in a specific frequency range, such as 500 Hz-4000 Hz.

Example 7

[0061] A vibration generation portion of a bone conduction speaker may be shown in FIG. 9-A. A transducer of the bone conduction speaker may include a magnetic circuit system including a magnetic flux conduction plate 910, a magnet 911 and a magnetizer 912, a vibration board 914, a coil 915, a first vibration conductive plate 916, and a second vibration conductive plate 917. The panel 913 may protrude out of the housing 919 and may be connected to the vibration board 914 by glue. The transducer may be fixed to the housing 919 via the first vibration conductive plate 916 forming a suspended structure.

[0062] A compound vibration system including the vibration board 914, the first vibration conductive plate 916, and the second vibration conductive plate 917 may generate a smoother frequency response curve, so as to improve the sound quality of the bone conduction speaker. The transducer may be fixed to the housing 919 via the first vibration conductive plate 916 to reduce the vibration that the transducer is transferring to the housing, thus effectively decreasing sound leakage caused by the vibration of the housing, and reducing the effect of the vibration of the housing on the sound quality. FIG. 9-B shows frequency response curves of the vibration intensities of the housing of the vibration generation portion and the panel. The bold line refers to the frequency response of the vibration generation portion including the first vibration conductive plate 916, and the thin line refers to the frequency response of the vibration generation portion without the first vibration conductive plate 916. As shown in FIG. 9-B, the vibration intensity of the housing of the bone conduction speaker without the first vibration conductive plate may be larger than that of the bone conduction speaker with the first vibration conductive plate when the frequency is higher than 500 Hz. FIG. 9-C shows a comparison of the sound leakage between a bone conduction speaker includes the first vibration conductive plate 916 and another bone conduction speaker does not include the first vibration conductive plate 916. The sound leakage when the bone conduction speaker includes the first vibration conductive plate may be smaller than the sound leakage when the bone conduction speaker does not include the first vibration conductive plate in the intermediate frequency range (for example, about 1000 Hz). It can be concluded that the use of the first vibration conductive plate between the panel and the housing may effectively reduce the vibration of the housing, thereby reducing the sound leakage.

[0063] The first vibration conductive plate may be made of the material, for example but not limited to stainless steel, copper, plastic, polycarbonate, or the like, and the thickness may be in a range of 0.01 mm-1 mm.

Example 8

[0064] This example may be different with Example 7 in the following aspects. As shown in FIG. 10, the panel 1013 may be configured to have a vibration transfer layer 1020 (for example but not limited to, silicone rubber) to produce a certain deformation to match a user's skin. A contact portion being in contact with the panel 1013 on the vibration transfer layer 1020 may be higher than a portion not being in contact with the panel 1013 on the vibration transfer layer 1020 to form a step structure. The portion not being in contact with the panel 1013 on the vibration transfer layer 1020 may be configured to have one or more holes 1021. The holes on the vibration transfer layer may reduce the sound leakage: the connection between the panel 1013 and the housing 1019 via the vibration transfer layer 1020 may be weakened, and vibration transferred from panel 1013 to the housing 1019 via the vibration transfer layer 1020 may be reduced, thereby reducing the sound leakage caused by the vibration of the housing; the area of the vibration transfer layer 1020 configured to have holes on the portion without protrusion may be reduced, thereby reducing air and sound leakage caused by the vibration of the air; the vibration of air in the housing may be guided out, interfering with the vibration of air caused by the housing 1019, thereby reducing the sound leakage.

Example 9

[0065] The difference between this example and Example 7 may include the following aspects. As the panel may protrude out of the housing, meanwhile, the panel may be connected to the housing via the first vibration conductive plate, the degree of coupling between the panel and the housing may be dramatically reduced, and the panel may be in contact with a user with a higher freedom to adapt complex contact surfaces (as shown in the right figure of FIG. 11-A) as the first vibration conductive plate provides a certain amount of deformation. The first vibration conductive plate may incline the panel relative to the housing with a certain angle. Preferably, the slope angle may not exceed 5 degrees.

[0066] The vibration efficiency may differ with contacting statuses. A better contacting status may lead to a higher vibration transfer efficiency. As shown in FIG. 11-B, the bold line shows the vibration transfer efficiency with a better contacting status, and the thin line shows a worse contacting status. It may be concluded that the better contacting status may correspond to a higher vibration transfer efficiency.

Example 10

[0067] The difference between this example and Example 7 may include the following aspects. A boarder may be added to surround the housing. When the housing contact with a user's skin, the surrounding boarder may facilitate an even distribution of an applied force, and improve the user's wearing comfort. As shown in FIG. 12, there may be a height difference do between the surrounding border 1210 and the panel 1213. The force from the skin to the panel 1213 may decrease the distanced between the panel 1213 and the surrounding border 1210. When the force between the bone conduction speaker and the user is larger than the force applied to the first vibration conductive plate with a deformation of do, the extra force may be transferred to the user's skin via the surrounding border 1210, without influencing the clamping force of the vibration portion, with the consistency of the clamping force improved, thereby ensuring the sound quality.

Example 11

[0068] The difference between this example and Example 8 may include the following aspects. As shown in FIG. 13, sound guiding holes are located at the vibration transfer layer 1320 and the housing 1319, respectively. The acoustic wave formed by the vibration of the air in the housing is guided to the outside of the housing, and interferes with the leaked acoustic wave due to the vibration of the air out of the housing, thus reducing the sound leakage.

[0069] The embodiments described above are merely implements of the present disclosure, and the descriptions may be specific and detailed, but these descriptions may not limit the present disclosure. It should be noted that those skilled in the art, without deviating from concepts of the bone conduction speaker, may make various modifications and changes to, for example, the sound transfer approaches described in the specification, but these combinations and modifications are still within the scope of the present disclosure.