阅读说明：本技术 包含多个振膜的多范围扬声器 (Multi-range loudspeaker comprising a plurality of diaphragms ) 是由 L·H·曹 Y·曹 C·菲姆里特 于 2020-02-18 设计创作，主要内容包括：公开了一种能够使用条形磁体、多个振膜、以及共享平面语音线圈来产生多频率范围声音的扬声器的实施例。平面语音线圈位于条形磁体之间,并且将接收到的电信号转变成使振膜振动的动能,从而再现多频率范围声音。在一些实施例中,扬声器生成双向声音。(Embodiments of a speaker capable of producing multiple frequency range sound using a bar magnet, multiple diaphragms, and a shared planar voice coil are disclosed. The planar voice coil is located between the bar magnets and converts the received electrical signal into kinetic energy that vibrates the diaphragm, thereby reproducing sound in multiple frequency ranges. In some embodiments, the speaker generates bidirectional sound.)

1. A loudspeaker, comprising:

a first bar magnet comprising a north pole and a south pole;

a second bar magnet comprising a north pole and a south pole, the second bar magnet being located a predetermined distance from and parallel to the first bar magnet, wherein the north pole of the second bar magnet faces the south pole of the first bar magnet and the south pole of the second bar magnet faces the north pole of the first bar magnet;

a voice coil plate located between the first bar magnet and the second bar magnet, the voice coil plate including a coil for receiving an electrical signal;

a first diaphragm attached to a first end of the voice coil board by a first connector; and

a second diaphragm attached to the first end of the voice coil board by a second connector;

wherein the voice coil plate vibrates the first diaphragm and the second diaphragm in response to a force generated by an electrical signal in the coil and a magnetic field between the first bar magnet and the second bar magnet.

2. The loudspeaker of claim 1, wherein the first diaphragm and the second diaphragm are of different sizes.

3. The loudspeaker of claim 2 wherein the first diaphragm is capable of reproducing sound in a first frequency range and the second diaphragm is capable of reproducing sound in a second frequency range different from the first frequency range.

4. The speaker of claim 1, further comprising:

a first yoke attached to a first side of the first bar magnet;

a second yoke attached to a first side of the second bar magnet;

a third yoke attached to a second side of the first bar magnet; and

a fourth yoke attached to a second side of the second bar magnet.

5. The speaker of claim 1, further comprising:

a frame that may enclose the speaker.

6. The speaker of claim 1, wherein the winding coil is attached to one or both sides of the voice coil plate.

7. The speaker of claim 1, wherein the voice coil board comprises a printed circuit board comprising etched coils, wherein etched coils are etched into a plurality of layers within the printed circuit board.

8. The loudspeaker of claim 7, wherein two or more of the plurality of layers are connected by one or more electrical vias to combine the etched coils of each layer in series or in parallel.

9. The speaker of claim 8, wherein one or more layers are attached to a control gate that can be opened or closed to alter the impedance of the speaker.

10. A loudspeaker, comprising:

a first bar magnet comprising a north pole and a south pole;

a second bar magnet comprising a north pole and a south pole, the second bar magnet being located a predetermined distance from and parallel to the first bar magnet, wherein the north pole of the second bar magnet faces the south pole of the first bar magnet and the south pole of the second bar magnet faces the north pole of the first bar magnet;

a voice coil plate located between the first bar magnet and the second bar magnet, the voice coil plate including a coil for receiving an electrical signal;

a first diaphragm attached to a first end of the voice coil board by a first connector;

a second diaphragm attached to the first end of the voice coil board by a second connector;

a third diaphragm attached to a second end of the voice coil board by a third connector; and

a fourth diaphragm attached to the second end of the voice coil board by a fourth connector;

wherein the voice coil plate vibrates the first diaphragm, the second diaphragm, the third diaphragm, and the fourth diaphragm in response to a force generated by an electrical signal in the coil and a magnetic field between the first bar magnet and the second bar magnet.

11. The loudspeaker of claim 10, wherein the first diaphragm, the second diaphragm, the third diaphragm, and the fourth diaphragm have different sizes.

12. The loudspeaker of claim 11, wherein the first diaphragm is capable of reproducing sound in a first frequency range, the second diaphragm is capable of reproducing sound in a second frequency range, the third diaphragm is capable of reproducing sound in a third frequency range, and the fourth diaphragm is capable of reproducing sound in a fourth frequency range; and is

Wherein the first frequency range, the second frequency range, the third frequency range, and the fourth frequency range are each different from one another.

13. The speaker of claim 10, further comprising:

a first yoke attached to a first side of the first bar magnet;

a second yoke attached to a first side of the second bar magnet;

a third yoke attached to a second side of the first bar magnet; and

a fourth yoke attached to a second side of the second bar magnet.

14. The speaker of claim 10, further comprising:

a frame that may enclose the speaker.

15. The speaker of claim 10, wherein the winding coil is attached to one or both sides of the voice coil plate.

16. The speaker of claim 10, wherein the voice coil board comprises a printed circuit board comprising etched coils, wherein the etched coils are etched into multiple layers within the printed circuit board.

17. The loudspeaker of claim 16, wherein two or more of the plurality of layers are connected by one or more vias to combine the etched coils of each layer in series or in parallel.

18. The speaker of claim 17, wherein one or more through-holes are attached to a control gate that can be opened or closed to alter the impedance of the speaker.

Technical Field

Embodiments of a speaker capable of producing multiple frequency ranges of sound are disclosed. The loudspeaker includes a bar magnet, a plurality of diaphragms, and one or more arrangements of coil-shaped conductors. Each configuration of coiled conductors is located between the bar magnets and converts the received electrical signals into kinetic energy that vibrates one or more diaphragms, each of which, if sized differently, is more suitable for producing sound in a different frequency range. In some embodiments, the speaker generates bidirectional sound.

Background

A schematic illustration of a conventional prior art cone loudspeaker 100 is shown in fig. 1. The cone type speaker 100 generally has a cylindrical shape, and uses a cylindrical permanent magnet 10. The cone loudspeaker 100 further comprises a voice coil 11, a diaphragm 12, a frame 13 and a damper 14. It is noteworthy that because diaphragm 12 is conical, it has a significant height, which may be more restrictive on the overall speaker structure. Furthermore, the T-yoke (T-yoke) 15 also has a significant height and may be more thin than necessary for the overall speaker structure.

Furthermore, the use of a cylindrical magnet 10 forces the frame to adopt a closed conical structure which, for practical reasons, is limited to having multiple diaphragms driven by the same voice coil. The prior art also includes coaxial speakers in which multiple cone speakers are contained in a common structure, such as a tweeter (tweeter) embedded within a woofer (woofer), but in those instances each speaker is driven by a separate voice coil and magnetic structure, rather than by the same voice coil and magnetic structure. Thus, in the prior art, the only existing multiple frequency range loudspeakers comprise two separate loudspeakers (having two diaphragms, each diaphragm being driven by a separate voice coil and magnet) combined into one structure, which results in a more complex structure and additional size and weight in the design.

Furthermore, to support the latest developments in three-dimensional surround sound systems or other kinds of different sound reproduction required by the industry, loudspeakers must be able to reproduce a wide range of sound signals with low distortion. The physical size of each diaphragm inherently limits the frequency range of sound that the diaphragm can effectively produce. A relatively small diaphragm cannot reproduce low frequency sound efficiently because the wavelength of the sound is larger than the diaphragm itself. On the other hand, relatively large diaphragms designed primarily to reproduce low frequency sounds may not be suitable for reproducing high frequency sounds because the larger prior art cone diaphragms are typically not stiff enough to reproduce high frequency sounds without diaphragm cracking and modal behavior, resulting in significant distortion. The prior art lacks efficient speaker structures that address both spatial constraints and the requirement for wide frequency range sound. One prior art solution is to use a plurality of loudspeakers arranged at different frequency ranges at a distance from each other, but this approach results in occupying an unnecessarily large space. Accordingly, there is a need for an improved loudspeaker that can effectively reproduce a wide range of sound frequencies, but occupies less space than prior art loudspeakers.

Disclosure of Invention

The present invention solves the limitations of prior art loudspeakers by providing loudspeakers as follows: the loudspeaker efficiently produces sound at multiple frequency ranges by using differently sized diaphragms while using less space than required by one prior art loudspeaker. By using a larger proportion of the outer surface of the loudspeaker, the multi-diaphragm loudspeaker of the present invention can achieve greater efficiency than similarly sized prior art loudspeakers. These embodiments maintain an ultra-thin form and produce a wide range of frequencies. These embodiments also provide design options for improved directional control of the reproduced sound.

In a multi-diaphragm embodiment of a loudspeaker, multiple diaphragms are coupled to the same voice coil board (also known as a bobbin) or Flexible Printed Circuit Board (FPCB) or any other material component. This provides the opportunity to include any number of sound generating surfaces above a single motor structure. These surfaces may have different surface areas, materials and curvatures to achieve different frequency bands and dispersions. Alternatively, the diaphragms may be coplanar or approximately coplanar. The distance between the diaphragms may be varied to achieve different purposes. Further, each diaphragm may take any shape, including but not limited to circular, elliptical, rectangular, etc.

Drawings

Exemplary embodiments of the invention are described with reference to the accompanying drawings, in which:

fig. 1 depicts a conventional loudspeaker having a conical structure.

Fig. 2 depicts an embodiment of a loudspeaker comprising a diaphragm and a pair of bar magnets.

Fig. 3a depicts a cross-sectional embodiment of the voice coil plate of fig. 2 viewed along the x-axis, wherein current flows in a first direction, as indicated by the standard "dot and cross" symbol.

Fig. 3b depicts a side view of the voice coil plate viewed along the z-axis of fig. 3 a.

Fig. 3c is a schematic cross-sectional view of the voice coil plate of fig. 3a, with current flowing in opposite directions, as indicated by the standard "dot and cross" symbols.

Fig. 3d depicts a side view of the voice coil plate viewed along the z-axis of fig. 3 c.

Fig. 4 depicts a multi-view embodiment of a speaker that may use a bar magnet, multiple diaphragms, and a shared voice coil to generate sound in multiple frequency ranges.

Fig. 5 illustrates the occurrence of local vibration due to low frequency long wavelength sound relative to the size of the diaphragm.

Fig. 6a is a three-dimensional partial view of a loudspeaker that can use a pair of bar magnets, multiple diaphragms, and a shared voice coil to generate sound in multiple frequency ranges.

Fig. 6B and 6c are cross-sectional views along the planes a-a 'and B-B', respectively, illustrated in fig. 6 a.

Detailed Description

The features and advantages of the present invention described above will become apparent from the following description taken in conjunction with the accompanying drawings. From the description, a person having appropriate technical expertise will be able to carry out the technical ideas explained in the present invention in the relevant industries. Since the present invention can have a variety of different applications, and can take different forms and shapes, only specific examples are illustrated by the figures and detailed description in the text. However, it is not intended to limit the invention to the particular forms disclosed; the intention is to cover all modifications, equivalents, and alternatives falling within the scope of the invention. The terminology used herein is for the purpose of describing particular examples only and is not intended to be limiting of the invention.

Fig. 2 depicts a loudspeaker design utilizing a single diaphragm and a pair of bar magnets. The speaker 200 includes bar magnets 110 and 110', upper yokes 120 and 120', lower yokes 130 and 130', a diaphragm 140, and a voice coil board 150. The speaker 200 further includes a speaker frame 160. The bar magnets 110 and 110' include a pair of bar magnets positioned with a predetermined distance therebetween such that different polarities face each other. At one end, the voice coil plate 150 is secured to the speaker frame 160 by the diaphragm 140, and at the other end, the voice coil plate 150 is secured to the speaker frame 150 by the damper 170 or by a second diaphragm (not shown).

The upper yokes 120 and 120 'are attached to the upper portions of the bar magnets 110 and 110' in the same plane, and the lower yokes 130 and 130 'are attached to the lower portions of the bar magnets 110 and 110' in the same plane. The upper yokes 120 and 120 'and the lower yokes 130 and 130' contain and guide the magnetic field in the region between the magnets in which the voice coil resides. The upper yokes 120 and 120' and the lower yokes 130 and 130' may optionally extend beyond the bar magnets 110 and 110' into the magnetic gap to increase the magnetic flux density induced in the magnetic gap. Further, the yokes 120 and 120 'may optionally comprise the same yoke, and the yokes 130 and 130' may optionally comprise the same yoke.

The diaphragm 140 is positioned either above the upper yokes 120 and 120 'or below the lower yokes 130 and 130'. In this case, the diaphragm 140 must be configured to generate a corresponding frequency range sound depending on the size of the diaphragm 140. In this embodiment, diaphragm 140 is substantially flat. However, the diaphragm 140 may instead be convex or concave, or any shape relative to the top surface of the frame designed for any application-dependent acoustic design.

Fig. 3a, 3b, 3c and 3d taken from the context of fig. 2 illustrate a method of operation of a loudspeaker. The voice coil board 150 must be positioned in a substantially rigid planar form in the gap between the bar magnets 110 and 110'. The coil 151/152 may be placed on one or both sides of the voice coil board 150. Diaphragm 140 will vibrate in a particular frequency range by the magnetic field induced by the pair of bar magnets 110 and 110' and the current flowing in coil 151/152.

During operation, coil 151/152 receives an electrical audio signal from signal source 210 through conductors 211 and 211'. A magnetic field is generally induced by the bar magnets 110 and 110' in a direction from the north pole (N) to the south pole (S). During the first half of the signal period (defined as the "positive half period"), current flows through coil 151 of fig. 3a "out of the page" and current flows through coil 152 "into the page" of fig. 3a, according to the standard "point and cross" convention for current flow through the plane of the page. This current flow direction is shown in fig. 3b from a different point of view. When the voice coil board 150 and the coupled voice coil 200 are installed in the context of fig. 2, lorentz forces are generated by both the coil 151 and the coil 152, the coil 151 interacting with the magnetic field between the top yokes 120 and 120', the coil 152 interacting with the magnetic field between the bottom yokes 130 and 130', wherein the forces align in the same direction and push the voice coil board 150 upwards, which pushes the diaphragm 140 upwards according to the magnitude of the electrical signal from the signal source. During the second half of the signal period (defined as the "negative half period"), current flows through coil 151 of fig. 3c "into the page" and current flows through coil 152 of fig. 3c "out of the page" according to the standard "point and cross" convention for current flowing through the plane of the page. Since the direction of the current in both 151 and 152 of the voice coil is reversed, the lorentz forces from the interaction with the magnetic field between 120, 120 'and 130, 130', respectively, will align in the same direction to push the voice coil plate 150 downwards, which pulls the diaphragm 140 downwards according to the magnitude of the electrical signal from the signal source.

In all embodiments of the speaker, both those already mentioned and those yet to be mentioned in this patent, each voice coil may be composed of any conductive material, including but not limited to copper wire, printed circuit board, flexible printed circuit board, or any variation of other conductive metal or alloy.

The diaphragm 140 may be connected to the frame 160 using a connector 153 shown in fig. 2, and the connector 153 may be made of a flexible material such as rubber, and connects the diaphragm 140 and the frame 160. Accordingly, an electrical audio signal from the signal source is converted into kinetic energy to move the diaphragm 140, thereby reproducing sound.

Fig. 4 depicts a loudspeaker 300, the loudspeaker 300 being one that is capable of producing sound in multiple frequency ranges using a bar magnet, multiple diaphragms, and a shared planar voice coil. Fig. 4 shows a top view, a cross-sectional view along a plane perpendicular to the magnetic gap (shown at the bottom of fig. 4), and a view of the removed voice coil plate assembly with respect to each other as indicated by the dashed lines (shown on the right side of fig. 4). The correct placement of the two diaphragms on the shared voice coil board in fig. 4 will result in the rendering of a loudspeaker that can reproduce sound in multiple frequency ranges.

The speaker 300 includes some components in common with the speaker 200 of fig. 2, namely bar magnets 110 and 110', upper yokes 120 and 120', and lower yokes 130 and 130 '. As in fig. 3b and 3d, signal source 210 generates an electrical audio signal that is provided to coil 151/152 through conductors 211 and 211'.

The speaker 300 further includes a diaphragm 340, a diaphragm 340', a voice coil plate 350, and a speaker frame 360. That is, two or more diaphragms 340 and 340' substantially in the same plane are attached to the top side of the voice coil board 350. Alternatively, this may be done using connectors 353 and 354, respectively. The resulting assembly is a multi-diaphragm loudspeaker, thereby reproducing different frequency ranges simultaneously, which allows for the reproduction of richer and more varied audio frequencies, since the loudspeaker structure is capable of reproducing multi-range sound.

The bar magnets 110 and 110' are positioned apart from each other by a predetermined distance with different polarities facing each other. The upper yokes 120 and 120 'are attached to the upper portions of the bar magnets 110 and 110', and the lower yokes 130 and 130 'are attached to the lower portions of the bar magnets 110 and 110'. The upper yokes 120 and 120' and the lower yokes 130 and 130' serve to control magnetic fluxes induced by the bar magnets 110 and 110 '. For this purpose, the upper yokes 120 and 120' and the lower yokes 130 and 130' have a larger width than the bar magnets 110 and 110', thereby concentrating the magnetic flux on the coil 151/152. Alternatively, yokes 120 and 120 'may be substantially the same piece in other embodiments of the invention, and alternatively yokes 130 and 130' may be substantially the same piece in other embodiments of the invention.

The first diaphragm 340 is attached to the voice coil plate 350 and positioned on an upper portion of the basin frame 360. The second diaphragm 340' is positioned substantially coplanar with the first diaphragm 340 and attached to the voice coil plate 350. Both the first diaphragm 340 and the second diaphragm 340' are positioned on an upper portion of the voice coil plate 350 and receive vibrational energy from the voice coil 150 in response to electrical current received in the voice coil 151/152.

In this example, the first and second diaphragms 340, 340 'are different in size, and thus the first and second diaphragms 340, 340' each reproduce a frequency range different from the other reproduced frequency range. The size of each diaphragm can be increased or decreased to produce either lower or higher frequency sound, which is roughly determined by the following equation:

whereinf ₀= cut-off frequency

Whereinc = speed of sound in air

Whereind = diaphragm size.

For example, by making the size of the first diaphragm 340 smaller than that of the second diaphragm 340', it is possible to make the first frequency range (which is the desired frequency range of the first diaphragm 340) higher than the second frequency range (which is the desired frequency range of the second diaphragm 340'). That is, as the size of the diaphragm becomes smaller, the frequency range that will be efficiently and accurately transmitted through the diaphragm will be made higher.

In the alternative, by making the size of the first diaphragm 340 larger than that of the second diaphragm 340', the frequency range of the first diaphragm 340 may be made lower than that of the second diaphragm 340'. That is, as the size of the diaphragm becomes larger, the desired frequency range to be efficiently and accurately transmitted through the diaphragm will become lower.

Voice coil plate 350 is positioned in a space between bar magnets 110 and 110 'in a plane perpendicular to a plane containing magnets 110 and 110', and one or more coils including elements 151 and 152 are coupled to one or both sides of voice coil plate 350. In response to the lorentz force generated by the interaction of the current flowing through the elements 151 and 152 including the voice coil and the magnetic field induced by the pair of bar magnets 110 and 110', the first diaphragm 340 will effectively vibrate in the first frequency range, and the second diaphragm 340' will effectively vibrate in the second frequency range.

The voice coil plate 350 may be connected to the first and second diaphragms 340 and 340'. The voice coil board 350 may optionally extend from a plane containing the first and second diaphragms 340 and 340 'to include a connector 353 (first joint) and a connector 354 (second joint) that connect the first diaphragm 340 and the second diaphragm 340' to the voice coil board 350, respectively. The connectors 353 and 354 allow vibrational energy generated by the lorentz forces derived from the current in the coil 151/152 interacting with the permanent magnetic field to be efficiently transferred to the first and second diaphragms 340 and 340'. In the standard top view of fig. 4, although the first and second joints are located below the diaphragms 340 and 340', these connectors are shown by the diaphragms 340 and 340' to clarify their respective connection points below each diaphragm, as indicated by the dashed lines.

Alternatively, the first and second diaphragms 340 and 340' may form part of an exterior of the sealed speaker frame and may be directly connected to the speaker frame 360 or may be indirectly connected through connectors, such as connectors 363 and 364.

The lorentz force is generated in the same manner as previously described for fig. 2, except that here the voice coil plate 350 acts on both diaphragms 340 and 340'.

Fig. 5 depicts the cause of local vibration with respect to low and high frequency signals based on diaphragm size. For example, assuming a sound velocity of 340m/s, if the first diaphragm 340 is 10cm wide at its maximum, the first frequency range will actually be 3400Hz or higher. If the second diaphragm 340' is 30cm at its maximum extent, the second frequency range will be about 1100Hz or higher. As a result, the first diaphragm 340 can successfully output a signal having a frequency higher than 3400Hz, but a signal lower than 3400Hz will cause local vibration of the first diaphragm 340 because the wavelength of the audio signal is larger than the diaphragm itself. Similarly, the second diaphragm 340 'may successfully output a signal having a frequency above about 1100Hz, but a signal below about 1100Hz will cause local vibration of the second diaphragm 340' since the audio signal generated has a wavelength longer than the diaphragm itself. The local vibration of the diaphragm results in distorted sound and inaccurate reproduction of sound from the signal source 210.

The size of the first and second diaphragms 340 and 340' may be described by their length along the x-axis and their width along the z-axis. Also, the shape of the diaphragms 340 and 340' may be circular, elliptical, rectangular, or any combination of these, and they may be flat, convex, or concave along the y-axis. In the example shown, the first and second diaphragms 340 and 340' are flat and have a minimum height along the y-axis, which is a significant difference from the diaphragm 12 in the loudspeaker 100, which allows the loudspeaker 300 to be thinner than the loudspeaker 100. These variations are optional and make them more practical to implement by the present invention.

As the size of the diaphragms 340 and 340 'increase along the x-axis and/or the z-axis, the distance between the diaphragms 340 and 340' may increase or decrease as desired. The distance between the diaphragms 140 and 140' may be determined based on interference or distortion effects between the first and second frequency ranges.

Fig. 6a, 6b and 6c contain detailed schematic illustrations of another practical example of a multi-frequency range loudspeaker using bar magnets. The loudspeaker 400 depicted in fig. 6a, 6b and 6c comprises: a plurality of diaphragms at the top of the loudspeaker and a plurality of diaphragms at the bottom of the loudspeaker, which together may play at least 4 different frequency ranges. Fig. 6a is a three-dimensional partial view of a loudspeaker 400, and fig. 6B and 6c are cross-sections along a-a 'and B-B', respectively, of a loudspeaker 400 comprising different diaphragms.

The speaker 400 includes a pair of bar magnets 210 and 210', top yokes 220 and 220', bottom yokes 230 and 230', a diaphragm 240, 240', 240 ″ and 240 ″ ', a voice coil board 250, and a speaker frame 260. Optionally, the speaker 400 further includes connectors 253 and 254, the connectors 253 and 254 being extensions of the voice coil plate 250 and being in contact with the diaphragms 240 and 240', respectively, and similar connectors (not shown) as extensions of the voice coil plate 250 being in contact with the diaphragms 240 ″ and 240 ″. The bar magnets 210 and 210', the top yokes 220 and 220', the bottom yokes 230 and 230', and the speaker frame 260 are identical to the bar magnets 110 and 110', the top yokes 120 and 120', the bottom yokes 130 and 130', and the speaker frame 160 and 360 of the speakers 200 and 300 of fig. 2 and 3, and operate according to the same principles as previously described in fig. 2 and 3.

As depicted in fig. 6a, 6b and 6c, the diaphragms 240, 240', 240 ″ and 240 "' have widths W1, W2, W3 and W4, respectively, which in this particular example are different from each other such that W4> W3> W2> W1. The width of the diaphragms 240, 240', 240 ", and 240"' may be modified to fit different frequency ranges. Here, the loudspeaker 400 includes four diaphragms, but it is understood that a smaller or larger number of diaphragms may be used.

For example, by increasing the size of the diaphragms 240, 240', 240 ", and 240'", it is possible to reduce the first through fourth frequency ranges, which allows the speaker to play a wider frequency range than the speaker 300 in fig. 3. On the other hand, by reducing the size of the diaphragms 240, 240', 240 ″ and 240 ″, it is possible to increase the frequency range. In the example depicted in fig. 6a, 6b and 6c, the first to fourth frequency ranges decrease, respectively, as the size of the first to fourth diaphragms (240, 240', 240 "') increases in order. In this case, the diaphragms 240, 240', 240 ″ and 240 ″' are vibrated by the shared voice coil plate 250.

Here, a signal to be output by the first diaphragm 240 may be controlled if an incoming signal frequency is higher than a first frequency range, a signal to be output by the second diaphragm 240 'may be controlled if the incoming signal frequency is between the first and second frequency ranges, a signal to be output by the third diaphragm 240 ″ may be controlled if the incoming signal frequency is between the second and third frequency ranges, or a signal to be output by the fourth diaphragm 240 ″' may be controlled if the incoming signal frequency is lower than the third frequency range.

In contrast, if the sizes of the first to fourth diaphragms 240, 240 'and 240' ″ are decreased in order (contrary to the manner shown in fig. 6a, 6b and 6 c), the first to fourth frequency ranges are increased, respectively. Here, a signal to be output by the first diaphragm 240 may be controlled if an incoming signal frequency is lower than a frequency range of the second diaphragm, a signal to be output by the second diaphragm 240' may be controlled if an incoming signal frequency is between frequency ranges of the second and third diaphragms, a signal to be output by the third diaphragm 240 ″ may be controlled if an incoming signal frequency is between frequency ranges of the third and fourth diaphragms, or a signal to be output by the fourth diaphragm 240 ″ may be controlled if an incoming signal frequency is higher than a third frequency range.

The lorentz forces are generated in the same manner as previously described for fig. 2, except that here the voice coil plate 250 acts on the diaphragms 240, 240', 240 "and 240"'.

According to the previously discussed example, unlike a conventional speaker such as the speaker 100, it is possible to realize a flat speaker of a rectangular shape instead of a circular speaker in order to simplify the components holding the voice coil board and the plurality of diaphragms, thereby playing multi-frequency range sounds simultaneously by varying the sizes of the diaphragms, and playing a wide range of sounds as a whole.

According to the present invention, the output direction of the speaker can be controlled by changing the direction of the current flowing in the voice coil plate, and the multi-frequency range sound can be effectively played by having diaphragms of different sizes.

According to the present invention, by placing differently sized diaphragms and adjusting the distance between the diaphragms, it is possible to achieve enhancement of sound pressure level and the ability to play multi-range sound while having an ultra-thin form.

The present invention allows the speaker to be ultra-light and ultra-thin, which perfectly meets the requirements for speakers used in thin and light objects.

The speaker proposed in the present invention can effectively generate multi-range sound by having a plurality of diaphragms with different sizes. The control signal that determines the appropriate signal frequency range and selects the appropriate diaphragm to output may be created by a controller or processor. Such a controller or processor responsible for creating the control signals may be implemented by a combination of hardware and software.

In a software implementation, not only the procedures and functions described in this document, but also each component and operation in the present invention may be implemented using an appropriate programming language. Each software module is responsible for one or more processes or functions described in this document. The implemented software codes may be stored in an electronic memory and executed by a controller or a processor.

With the present invention, sound with a wide frequency range can be reproduced efficiently by stimulating the voice coil(s) with an AC electrical signal and by implementing differently sized diaphragms coupled to the voice coil(s) and moving accordingly. This type of speaker can be miniaturized and optimized to produce a desired sound output even in products requiring an ultra-thin form factor. Furthermore, the distance between the diaphragms may be determined to account for any interference or distortion effects between the selected frequency ranges for each diaphragm.

There are several opportunities to use this technology across many industries. For example, automobiles, or even other types of vehicles (such as boats, trains, and airplanes) may benefit from the ability to: that is, the multiple frequency ranges are closely collocated (co-located) in order to effectively cover the entire auditory spectrum, all while maintaining an ultra-thin form factor. Furthermore, home IoT products may enjoy more efficient coplanar integration of broadband sound produced by multiple diaphragms. Finally, "hi-fi" home audio systems may benefit from a new configuration that provides options for more aesthetically pleasing design and flexibility given spatial considerations.

Another advantage provided by embodiments is naturally efficient broadband frequency coverage. As in conventional loudspeakers, the frequency range capability of a loudspeaker depends to a large extent on the surface area, shape and material of the diaphragm. However, in conventional designs, the face of each speaker must be designed separately to cope with different frequency ranges. The multi-diaphragm structure allows diaphragm surfaces having different lengths and widths to be included in the same loudspeaker motor structure. By their nature of being directly attached to the voice coil via glue or another method, they can be designed as coplanar or otherwise similarly powered in-phase (in-phase) surfaces. However, these surfaces are designed differently and are all powered by the movement of a magnet and voice coil motor structure.

Yet another advantage provided by embodiments is the cooperative variation of surface design. Conventional sound systems typically implement different speaker drivers with different surface materials to achieve different properties. The loudspeakers are mounted as separate components in such a way that they can cooperate to achieve a higher overall sound quality than the individual components. However, the limitation is that: in order to use these different materials, multiple speaker drivers must be used. There are several design variations, such as dust cover designs and multi-axis speakers, but they still include multiple electromechanical motors for different speakers within their structure. With the present invention, in order to improve the original speaker structure, the multiple diaphragms may be implemented with different materials and different curvatures, in addition to the configuration of the multiple diaphragms and the attachment to the voice coil board. One surface may for example be designed as a soft dome tweeter, while the other surface is designed of a hard material for a subwoofer. Additionally, the materials and arrangements of the various surfaces may be interpreted to affect only the center of mass of the moving parts, or the entire system.

A final advantage provided by embodiments is the control of sound directionality. The end use of a speaker often requires a particular type of directivity, such as wide dispersion, narrow dispersion, or some sort in between. Whether the goal is to focus the sound in one particular direction or to broaden its dispersion, the surface orientation and curvature may provide better control of the sound directivity.

The foregoing merely illustrates the principles of the disclosure. Various modifications and alterations to the described embodiments will be apparent to those skilled in the art in view of the teachings herein. It will thus be appreciated that those skilled in the art will be able to devise numerous systems, arrangements and processes which, although not explicitly shown or described herein, embody the principles of the disclosure and are thus within its spirit and scope. As will be appreciated by one of ordinary skill in the art, the various exemplary embodiments may be used with each other and interchangeably. Furthermore, certain terms used in this disclosure (including their description, drawings, and claims) may be used synonymously in certain instances, including but not limited to, for example, data and information. It should be understood that although these terms and/or other terms that may be synonymous with one another may be used synonymously herein, there may also be instances when such terms may not be intended to be used synonymously. Further, to the extent that prior art knowledge has not been explicitly incorporated by reference herein above, it is explicitly incorporated herein in its entirety. All publications cited are incorporated herein by reference in their entirety.