Patent Application
20240284118
The present invention relates to a SoT module comprising a piezoelectric element formed in a rectangular plate.
In the acoustic field, a dynamic speaker configured by a coil are generally used. Although a dynamic speaker can generate sufficient sound pressure even in the low audio frequency range, the application is limited since the weight, the volume and the power consumption of the dynamic speaker are large. On the other hand, the application of the piezoelectric speaker using the piezoelectric element has been advanced (e.g., see Patent Document 1). Since the volume, the weight and the power consumption of a piezoelectric speaker are small, the piezoelectric speaker can also be used in applications difficult to apply dynamic speakers.
However, in the piezoelectric speaker, it is difficult to obtain a sufficient sound pressure in the low and middle audio frequency range. As a result, the sound pressure as a whole is often reduced. If the demerit is overcome, the piezoelectric module can be applied not only to speakers for watching television programs, movies, music, and the like, but also to various applications. A piezoelectric module that can obtain sufficient sound pressure in the low and middle audio frequency range is available for a loudspeaker and noise canceller, even if it does not have an acoustic structure such as a hole and cavity, as long as it has a vibration plate.
Such a piezoelectric module has the potential to be quite different from a conventional piezoelectric module and should be referred to as a SoT (Sound of Things) module (hereinafter, piezoelectric modules that can improve sound pressure in a particular audio frequency range are referred to as a SoT module).
From the above circumstances, the inventors of the present invention have continued trial and error in the development of a piezoelectric module by which sufficient sound pressure is obtained even in the low and middle audio frequency range. For example, in the piezoelectric module 2100 shown in
Also, an attempt to increase the sound pressure by providing a plurality of piezoelectric elements has been made. In the piezoelectric module 3100 shown in
The present invention has been made in view of such circumstances, a SoT module that generates sufficient sound pressure in the low and middle audio frequency range and can be applied to a variety of applications is provided.
To achieve the above object, SoT module comprises a plate-shaped piezoelectric composite for generating bending vibration by the impression of an AC voltage, a plurality of elastic bodies, one ends of which are bonded to the main surface of the piezoelectric composite, the elastic bodies transmitting vibration of the piezoelectric composite and a vibration plate has a main surface which is bonded to the other ends of the elastic bodies, wherein the piezoelectric composite comprises a piezoelectric element formed in a rectangular plate, and there is a position of the centroid of the piezoelectric composite between the plurality of elastic bodies. Thus, the stiffness of the entire module can be reduced, and the displacement amplitude of the vibration plate can be increased. As a result, sufficient sound pressure is obtained in the low and middle audio frequency range, and it can be applied to various applications.
Next, embodiments of the present invention are described with reference to the drawings.
The piezoelectric elements 110a and 110b are arranged in parallel and are not connected to each other. Between the elastic bodies 120a and 120b is the position of the centroid of each of the piezoelectric elements 110a and 110b. As a result, sufficient sound pressure is obtained in the low and middle audio frequency range, SoT module 100 can be applied to a variety of applications. Each of the piezoelectric elements 110a and 110b configures a piezoelectric composite.
The piezoelectric bodies 111 and 112 are preferably formed of a piezoelectric ceramic material. As the piezoelectric material, for example, zirconate titanate (Pb(Ti, Zr)O3, so-called PZT) or barium titanate (BaTiO3) is used. Both are ferroelectrics, and PZT is preferable from the viewpoint of efficiency, but barium titanate is preferable from the viewpoint of lead-free. The piezoelectric bodies 111 and 112 may be formed of a piezoelectric polymer. Piezoelectric polymers comprise polyvinylidene fluoride and copolymers thereof, polylactic acid, polyvinylidene cyanide, polyurea and odd nylon.
Piezoelectric body 111 is polarized in the direction of the shim n plate 115 from the electrode 113, the piezoelectric body 112 is polarized in the direction of the electrode 114 from the shim plate 115. One electrode is connected to the electrodes 113 and 114, and the other electrode is connected to the shim plate 115. In this configuration, when an AC voltage is impressed to the piezoelectric bodies 111 and 112 by the power supply P1, one contracts and the other extends along a direction parallel to the surface by the reverse piezoelectric effect, and then the bending vibration occurs by repeating the movement shown as the arrow S1 and S2 in
The above-described piezoelectric element 110 has a parallel bimorph structure in which the polarization directions of the piezoelectric bodies 111 and 112 are the same but may have a series bimorph structure in which the polarization directions are different. Further, an insulator may be used for the central shim plate. The piezoelectric element 110 preferably has a bimorph structure but may have a unimorph structure. Further, for the piezoelectric element 110, a piezoelectric multilayer body may be used in place of the piezoelectric body of a single plate. In this case, an external electrode may be used, or an electrode may be formed by a via structure. Further, the piezoelectric element 110 is formed by the piezoelectric layer and the electrode being stacked, it may be a stretching-type piezoelectric element which expands and contracts in the stacking direction.
The elastic body 120a has one end bonded to the main surface of the piezoelectric element 110a and the other end bonded to the main surface of the vibration plate 130, and the elastic body 120b has one end bonded to the main surface of the piezoelectric element 110b and the other end bonded to the main surface of the vibration plate 130. For example, an epoxy-based, acrylic-based, or urethane-based adhesive can be used for bonding (hereinafter, for any bonding is the same). The elastic bodies 120a and 120b are preferably formed of a resin such as urethane. The elastic modulus of the elastic bodies 120a and 120b is preferably 70 MPa or more and 690 MPa or less. The elastic bodies 120a and 120b transmit the displacement of the piezoelectric elements 110a and 110b to the vibration plate 130.
Between the elastic bodies 120a and 120b, the position of the centroid for each of the piezoelectric elements 110a and 110b is preferably located. Thus, the stiffness of the entire SoT module 100 can be reduced, and the peak dip in the middle audio frequency range occurred for the piezoelectric elements 110a and 110b in which the natural frequency is set to be small can be eliminated. It is particularly preferable that the elastic bodies 120a and 120b are bonded to respective ends of the piezoelectric elements 110a and 110b. For each of the piezoelectric elements 110a and 110b, the region can be divided into a central portion, two intermediate portions, and two end portions.
Each of the elastic bodies 120a and 120b is preferably formed in a rectangular shape as shown in
The vibration plate 130 is formed in a plate shape and bonded to the elastic bodies 120a and 120b. The material of the vibration plate 130 varies depending on the application. For example, a styrene board can be used as the vibration plate 130. Further, it is possible to use a OLED panel as the vibration plate 130 of the TV speaker. Although the vibration plate 130 made of resin is easily used, a vibration plate with inelasticity enhanced using wood or fiber structure may be used.
The vibration plate 130 vibrates in the thickness direction by the displacement force transmitted through the elastic bodies 120a and 120b, vibrates air and generates sound waves. Depending on the frequency of the signal and the intensity of the current applied to the piezoelectric elements 110a and 110b, the pitch and the sound pressure of the sound generated from the vibration plate 130 appear differently for magnitude. In order to generate a large sound pressure, it is effective to improve the efficiency of vibration which is connected to the vibration plate.
The operation of the SoT module 100 is described below. By the electrical signal for the sound amplified by the amplifier being input to the SoT module 100, the piezoelectric composite 105 vibrates. Then, the displacement due to the vibration is transmitted to the vibration plate 130 via the elastic bodies 120a and 120b, and the vibration plate 130 vibrates to generate a sound corresponding to the electric signal.
The unconnected piezoelectric elements 110a and 110b are preferably driven in anti-phase or in-phase. The stiffness of the whole path transmitted by vibration and a combination of the phase driving each piezoelectric element is determined according to the required characteristics such as the sound pressure in the low audio frequency range. The stiffness of the whole path is determined by each element. For example, even when the stiffness of the piezoelectric elements 110a and 110b and the vibration plate 130 is large, when the stiffness of the elastic bodies 120a and 120b is small, the stiffness of the whole path may be small.
Although the independent two piezoelectric elements are arranged in parallel in the above embodiment, the piezoelectric elements installed in parallel may be connected by connecting members.
The SoT module 200 comprises piezoelectric elements 210a and 210b, elastic bodies 220a and 220b, connecting members 240a and 240b and a vibration plate 130. The piezoelectric elements 210a and 210b have the same configuration as the piezoelectric elements 110a and 110b, respectively. However, the piezoelectric elements 210a and 210b are provided in parallel with each other on the vibration plate 130, and a part of each other is connected to configure a plate-shaped piezoelectric composite 205. Thus, the vibration is amplified through the connecting portion, the displacement amplitude of the vibration plate 130 can be increased. Each of the elastic bodies 220a and 220b is formed of the same material in a rectangular plate shape and arranged as each of the elastic bodies 120a and 120b.
Each of the two connecting members 240a and 240b is formed of resin such as PET in a flat plate shape and connects the end of the piezoelectric element 210a and the end of the piezoelectric element 210b. The connecting is performed by bonding the back surfaces of the connecting members 240a and 240b and the surfaces of the piezoelectric elements 210a and 210b to each other. The connecting members 240a and 240b are arranged so that their longitudinal directions do not intersect each other and are preferably parallel to each other. The thickness of the connecting members 240a and 240b is designed according to the overall configuration, for example, 100 μm or more and 1000 μm or less. The piezoelectric elements 210a and 210b and the connecting members 240a and 240b configure the piezoelectric composite 205. In the cross-sectional view, the electrodes of the piezoelectric elements 210a and 210b are omitted.
It is preferable that the piezoelectric elements 210a and 210b are wired so as to be driven in in-phase or anti-phase to each other. That is, the piezoelectric elements 210a and 210b are wired so as to be driven in in-phase or anti-phase, and electric signals are input thereto. Thus, vibration of the piezoelectric elements 210a and 210b can be amplified via the connecting members 240a and 240b, and the sound pressure in the low audio frequency range to the middle audio frequency range can be improved. Either in-phase or anti-phase may be selected depending on the combination of the required characteristics and the stiffness of the whole path transmitted by the vibration.
For example, the piezoelectric elements 210a and 210b are wired so as to be driven in anti-phase to each other, and electric signals can be input. The respective piezoelectric elements 210a and 210b are driven in anti-phases with respect to the SoT module 200 in which the piezoelectric composite 205 is located on the upper side and the vibration plate 130 is located on the lower side. In this case, when the central portion of the piezoelectric element 210a is displaced downward, the central portion of the piezoelectric element 210b is displaced upward.
The piezoelectric elements 210a and 210b may be wired so as to be driven in phase with each other, and electric signals may be input. In the case that each piezoelectric element is driven in phase, when the center portion of the piezoelectric element 210a is displaced downward, the center portion of the piezoelectric element 210b is also displaced downward. When the central portion of the piezoelectric element 210a is displaced upward, the central portion of the piezoelectric element 210b is also displaced upward.
The SoT module 200 is preferably driven by a drive method for increasing the sound pressure of the low audio frequency range. When the displacement of the piezoelectric composite 205 with respect to the position is represented by a curve and the curve is overlapped with the one in anti-phase, there is a position where the curves intersect. This position would be called a displacement point, and the displacement point can be changed closer to or farther from the elastic bodies 220a and 220b by adjusting the drive signals (the anti-phase or in-phase). This adjustment allows amplification of sound pressure at a specific frequency. In this way, a sufficient sound pressure can be obtained even in the low audio frequency range, for example.
In the second embodiment, although the rectangular plate-shaped elastic body is provided only at the positions of both end portions of the piezoelectric element, the elastic body may be provided over the entire vibration plate. The elastic body may have a uniform plate shape or may be formed in a predetermined pattern as described later.
On the other hand, the elastic body 320 is formed in a uniform plate shape over the entire vibration plate 130. Thus, since the elastic body 320 is easily arranged, the stiffness of the SoT module 300 can be reduced by the elastic body 320 while the manufacturing load is reduced. The operation of the SoT module 300 is the same as that of the SoT module 200.
The elastic body 420 has a constant pattern shape over a cross section perpendicular to the thickness direction over the entire vibration plate 130. The constant pattern shape is preferably a shape in which a plurality of cylindrical holes are arranged periodically. Further, it is more preferable that a plurality of types of cylindrical holes having different diameters are provided. Thus, the constraint to the piezoelectric composite 205 becomes loose, and the displacement is not hindered. As a result, the stiffness S value of the whole system can be lowered, and the damping ratio of the vibration transmission path can be optimized.
The elastic body 420 has a constant pattern shape on a cross section perpendicular to the thickness direction over the entire vibration plate 130. The constant pattern shape is preferably a shape in which a plurality of spherical projections or cylinders are arranged periodically. Thus, the constraint to the piezoelectric composite 205 becomes loose, and the displacement is not hindered. As a result, the stiffness S value of the whole system can be lowered, and the damping ratio of the vibration transmission path can be optimized.
Although two piezoelectric elements are used in the above embodiment, three piezoelectric elements may be connected for the SoT module. In that case, the central portion of the SoT module installed in parallel can be connected by a piezoelectric element.
The piezoelectric elements 610a and 610b are configured in the same manner as the piezoelectric elements 210a and 210b, respectively. The elastic bodies 620a and 620b are formed of the same material and are arranged in the same manner as the elastic bodies 120a and 120b. The elastic bodies 620a and 620b support the piezoelectric elements 610a and 610b on the vibration plate 130, respectively, and transmit vibrations of the piezoelectric elements 610a and 610b to the vibration plate 130.
The piezoelectric element 610c has the same configuration as the piezoelectric element 610a and connects the center portions of the piezoelectric elements 610a and 610b. The connection is made by bonding the back surface of ends of the piezoelectric element 610c and the surface of the center portion of the piezoelectric elements 610a and 610b.
The wiring may be configured so that the piezoelectric elements 610a and 610b can be driven in anti-phases to the piezoelectric element 610c each other, and an electric signal may be input.
when the curves of the displacements of the piezoelectric composite 605 in anti-phases are overlapped and the position where the curves intersect is called a displacement point, the displacement point can be changed closer to or farther from the elastic bodies 620a and 620b by adjusting the drive signal (anti-phase or in-phase). This adjustment allows amplification of sound pressure at a specific frequency. By thus amplifying the displacement of the piezoelectric composite 605 and transmitting vibration to the vibration plate 130, it is possible to improve the sound pressure of the low audio frequency range.
In the above embodiments, there is a termination in the amplification path of the displacement of the piezoelectric element, but the SoT module may have a structure for amplifying the displacement in a loop. In the following example, four piezoelectric elements are used from the viewpoint of efficiency, but other numbers of piezoelectric elements such as three or five may be used.
The connection is performed, for example, by bonding the back surface of one end of the piezoelectric element 710a and the front surface of the center portion of the piezoelectric element 710b. A region surrounded by a dotted line in
The elastic bodies 720a to 720d are made of the same material as that of the elastic body 120a. As described above, one end of the piezoelectric element 710a is connected to the center portion of the other piezoelectric element 710b, and the other end is supported by the elastic body 720a. In this manner, the elastic bodies 720a to 720d support the ends of the piezoelectric elements 710a to 710d on the vibration plate 130, respectively and transmit the vibrations of the piezoelectric elements 710a to 710d to the vibration plate 130. The piezoelectric elements 710a to 710d are driven in in-phase or anti-phase, and the driving method thereof is set according to the stiffness of the entire path through which the vibrations are transmitted. The sound pressure can be amplified at a specific frequency by adjusting the drive signal (anti-phase or in-phase) to change the displacement point closer to or farther away from the elastic bodies 720a to 720d.
In the seventh embodiment, the connecting destination of one end of the piezoelectric element is a central portion of the other piezoelectric element, but an intermediate portion between the central portion and the end portion may be the destination.
In the seventh embodiment, the connecting destination of one end of the piezoelectric element is a central portion of the other piezoelectric element, an end portion may be the destination.
The piezoelectric elements may be connected so as to cross each other in the longitudinal direction to configure a piezoelectric composite. For example, the piezoelectric elements are arranged to intersect each other in the longitudinal direction and overlap the central portions. Then, the back surface of the central portion of the one piezoelectric element is bonded to the surface of the central portion of the other piezoelectric element. Thus, the displacement of the vibration plate can be amplified, and especially, the sound pressure in the middle audio frequency range from the low audio frequency range can be improved. It is preferable that the crossing is made at an orthogonal angle or an angle at which an effect equivalent thereto can be obtained.
In the above embodiment, the bending-type piezoelectric element is used, but a stretching-type piezoelectric element may be used. As the stretching-type piezoelectric element, it is preferable to use a piezoelectric element obtained by stacking a piezoelectric body and an electrode in the expansion direction.
The SoT module 1000 is configured of piezoelectric elements 1010, 1080, an elastic body 1020 and a vibration plate 130. Each of the piezoelectric elements 1010 and 1080 is a stretching-type piezoelectric element. The piezoelectric elements 1010 and 1080 are preferably formed by electrodes and piezoelectric bodies which are formed of piezoelectric ceramics polarized being stacked. The piezoelectric elements 1010 and 1080 generate stretching vibration by the impression of an AC voltage.
The piezoelectric elements 1010 and 1080 are alternately arranged in a single row along the longitudinal direction, by their end portions being connected to each other, to form steps of up and down. Specifically, the back surface of the piezoelectric element 1080 is bonded to the surface of the piezoelectric element 1010 at each of the ends. The piezoelectric elements 1010 are located in a state where a portion overlaps with the piezoelectric element 1080 each other on both sides of the piezoelectric element 1080 located in the center. The piezoelectric elements 1010 and 1080 configure the symmetrical piezoelectric composite 1005.
The plurality of piezoelectric elements 1010 and 1080 may be driven by an input of a single signal (in-phase drive) or may be driven by different signals by shifting the phase for a central piezoelectric element 1080 relative to the phase of the piezoelectric elements 1010 on both sides. The displacement of the piezoelectric composite 1005 with respect to the position is represented by a curve and the curve is overlapped with the one in anti-phase, there is a position where the curves intersect. The sound pressure can be amplified at a specific frequency by adjusting the drive signal (anti-phase or in-phase) to change the displacement point closer to or farther away from the elastic bodies 1020. In this manner, the amount of displacement can be amplified through the connecting portion. When only piezoelectric element 1080 is driven in a shifting the phase, it is preferably driven in anti-phase with the piezoelectric element 1010 on both sides.
The plurality of piezoelectric elements 1280 and 1210a to 1210d may be driven with a single signal input (in-phase drive) or may be driven with different signals in which the phase for the center piezoelectric element 1280 is out of the phase for the peripheral piezoelectric elements 1210a to 1210d. When only the piezoelectric element 1280 is driven in a shifted phase, it is preferably driven in anti-phase with the peripheral piezoelectric elements 1210a to 1210d. The sound pressure can be amplified at a specific frequency by adjusting the drive signal (anti-phase or in-phase) to change the displacement point closer to or farther away from the elastic bodies 1220a to 1220d.
The central piezoelectric element may be connected to the vibration plate side of the peripheral piezoelectric elements. Further, each of the connecting portions may be shifted to one side from the plane passing through the center of the central piezoelectric element.
The SoT module 2200 comprises a piezoelectric composite 2205, elastic bodies 2220a to 2220d, and a vibration plate 130. The piezoelectric composite 2205 comprises a central piezoelectric element 2280 and peripheral piezoelectric elements 2210a-2210d whose ends are connected to the edges of the central piezoelectric element 2280. The width of the central piezoelectric element 2280 is larger than the width of the peripheral piezoelectric elements 2210a to 2210d. The central piezoelectric element 2280 is connected to the vibration plate 130 side of the peripheral piezoelectric elements 2210a to 2210d. The connection direction of the piezoelectric elements 2210a, 2280, and 2210c connected in one row intersects the connection direction of the piezoelectric elements 2210b, 2280, and 2210d connected in another row at perpendicular angle at the center.
Each of the connecting portion is shifted to one side from the plane passing through the center of the central piezoelectric element 2280. For example, the connecting position of the piezoelectric element 2210d with respect to the plane P1 is shifted toward the piezoelectric element 2210a, and the connecting position of the piezoelectric element 2210b is shifted toward the piezoelectric element 2210c. In this way, the SoT module 2200 is formed in a windmill-like shape.
The plane P1 is a bisecting plane that evenly divides the piezoelectric composite 2205, and the piezoelectric composite 2205 is formed such that the shapes of both sides divided by the plane P1 are point symmetric with respect to one point on the plane P1. That is, the piezoelectric composite 2205 has a shape which looks inverted vertically and horizontally when viewed from one side to the other side divided by the plane P1. The piezoelectric composite 2205 has the same symmetry not only with respect to the plane P1 but also with respect to a bisecting plane (e.g., the plane P2) that divides evenly regardless of the angle.
The plurality of piezoelectric elements 2280 and 2210a to 2210d may be driven with a single signal input (in-phase drive) or may be driven with different signals in which the phase for the center piezoelectric element 2280 is out of the phase for the peripheral piezoelectric elements 2210a to 2210d. When only piezoelectric element 2280 is driven by shifting the phase, it is preferable to drive the piezoelectric elements 2210a to 2210d on peripheral region in anti-phase. The sound pressure to be amplified at a specific frequency by adjusting the drive signal (anti-phase or in-phase) to change the displacement point closer to or farther away from the elastic bodies 2220a to 2220d. Such adjustment is facilitated by the symmetry described above.
In the tenth to twelfth embodiments, the ends of the stretching-type piezoelectric elements are connected by bonding, but they may be connected via a base plate.
The SoT module 1300 comprises a piezoelectric element 1310 and 1390, elastic bodies 1320, a base plate 1360 and a vibration plate 130. Each of the piezoelectric elements 1310 and 1390 is a stretching-type piezoelectric element. The piezoelectric elements 1310 and 1390 are preferably formed by electrodes and piezoelectric bodies which are formed of piezoelectric ceramics polarized being stacked. The piezoelectric elements 1310 and 1390 generate stretching vibration by the impression of an AC voltage.
The piezoelectric elements 1310 and 1390 are provided in a row along the longitudinal direction on a rectangular base plate 1360. The piezoelectric elements 1310 and 1390 are alternately arranged at uniform intervals, and the piezoelectric composite 1305 is symmetrically formed. The piezoelectric elements 1310 and 1390 configure a symmetrical piezoelectric composite 1305.
The plurality of piezoelectric elements 1310 and 1390 may be driven by an input of a single signal (in-phase drive) or may be driven by different signals by shifting the phase for a central piezoelectric element 1390 relative to the phase of the piezoelectric elements 1310 on both sides. The displacement of the piezoelectric composite 1305 with respect to the position is represented by a curve and the curve is overlapped with the one in anti-phase, there is a position where the curves intersect. The sound pressure can be amplified at a specific frequency by adjusting the drive signal (anti-phase or in-phase) to change the displacement point closer to or farther away from the elastic bodies 1320. In this manner, the amount of displacement can be amplified through the connecting portion. The same effect can be obtained even when the elastic bodies 1320 and the vibration plate 130 are omitted and the base plate 1360 is used as the vibration plate.
The sound pressure can be amplified at a specific frequency by adjusting the drive signal (anti-phase or in-phase) to change the displacement point closer to or farther away from the elastic bodies 1320. Further, since the piezoelectric composites 1405a and 1405b are arranged in parallel, the amount of displacement can be amplified. The driving of the piezoelectric composites 1405a and 1405b can be performed in the same manner as the driving of the piezoelectric composite 1305.
In the piezoelectric composite 1505, a central piezoelectric element 1590 and peripheral piezoelectric elements 1510a to 1510d are located on a cross-shaped base plate 1560. The peripheral piezoelectric elements 1510a to 1510d are all formed in the same size. In an example shown in
The plurality of piezoelectric elements 1510a to 1510d and 1590 may be driven by an input of a single signal (in-phase drive) or may be driven by different signals by shifting the phase for a central piezoelectric element 1590 relative to the phase of the peripheral piezoelectric elements 1510a to 1510d. When only the piezoelectric element 1590 is driven in a shifted phase, it is preferably driven in anti-phase with the peripheral piezoelectric elements 1510a to 1510d. The sound pressure can be amplified at a specific frequency by adjusting the drive signal (anti-phase or in-phase) to change the displacement point closer to or farther away from the elastic bodies 1520a to 1520d.
The SoT module may be configured of a structure having a high thermal conductivity.
The SoT module 1600 comprises piezoelectric elements 1610a and 1610b, a base plate 1660, elastic bodies 1620, and a vibration plate 130. The two piezoelectric elements 1610a and 1610b and the base plate 1660 bonded thereto configure a piezoelectric composite 1605. The base plate 1660 is preferably formed of metal.
Each of the piezoelectric elements 1610a and 1610b has an element structure similar to that of the piezoelectric element 110a. The elastic bodies 1620 supports the base plate 1660 on the vibration plate 130 in the same material and arrangement as the elastic bodies 420 and transmits the vibration of the piezoelectric composite 1605 to the vibration plate 130. Since one end of the elastic body 1620 is bonded to the base plate 1660, heat accumulated in the piezoelectric elements 1610a and 1610b can be discharged.
The elastic body 1620 is preferably formed of an elastomer. Further, the elastic body preferably has a thermal coefficient of 1×10−4 cal·s−1cm−2 or more. Thus, the elastic body 1620 can discharge heat with high thermal conductivity.
The SoT module of the sixteenth embodiment is configured of piezoelectric elements, a base plate, elastic bodies and a vibration plate, but it may further have a partition.
The SoT module 1700 comprises a piezoelectric element, an elastic body 1720, a vibration plate 130 and a partition 1770. The piezoelectric element has the same element structure as the piezoelectric element 110. The piezoelectric elements are preferably connected to each other. The plurality of piezoelectric elements are separated to the left and right to form the piezoelectric composites.
The elastic body 1720 has one end bonded to the piezoelectric composite and the other end bonded to the vibration plate 130, and an assembly of the elastic bodies 1720 is formed for each of the two piezoelectric composites. Between them, the partition 1770 is provided. By the partition 1770, the acoustic interference in the left and right speakers can be suppressed.
The partition may have a structure surrounding the assembly of the elastic bodies.
The SoT module 1800 is configured in the same manner as the SoT module 1700 except that partitions 1870a and 1870b are provided instead of the partition 1770.
The partitions 1870a and 1870b surround assemblies of left and right elastic bodies 1720, respectively. The partitions 1870a and 1870b are configured of inner partitions 1871a and 1871b and outer partitions 1872a and 1872b, respectively. Since the partitions 1870a and 1870b have double structures surrounding the elastic bodies 1720, the sound is hardly transmitted to the outside of each of the partitions. Thus, it is possible to effectively suppress the acoustic interference occurring inside the left and right respective speakers.
The partition may have an air flow path.
The SoT module 1900 is configured in the same manner as the SoT module 1800 except that the partitions 1870a and 1870b are replaced with partitions 1970a and 1970b.
The partitions 1970a and 1970b are provided so as to surround respective assemblies of the left and right elastic bodies 1720. The partitions 1970a and 1970b are configured of inner partitions 1971a and 1971b and outer partitions 1972a and 1972b, respectively. The partitions 1970a and 1970b have double structures surrounding the elastic bodies 1720.
The inner partitions 1971a and 1971b have openings 1973a and 1973b and walls 1974a and 1974b, respectively. The outer partitions 1972a and 1972b also have walls 1975a and 1975b and openings 1976a and 1976b, respectively. Thus, a continuous air flow path is formed from the elastic body 1720 to the outside of the partitions 1970a and 1970b. As a result, the SoT module 1900 can improve the cooling efficiency while suppressing acoustic interference.
The SoT module configured as described above can be used in various applications. The applications can be roughly classified into acoustic and noise cancellation. Noise cancellation is a technique that uses sounds with anti-phases and is particularly effective for removing regular noise such as motor sounds. Though it is said to be difficult to cancel the noise of 1 kHz or less, the SoT module can also sufficiently work for the noise cancellation of 1 kHz or less.
If there is a plate which functions as a vibration plate, the SoT module can be configured by installing the piezoelectric elements and the elastic bodies there. For example, parts of plastic panels of automobile doors, ceilings, trunks, headrests, and dashboards can be utilized as vibration plates to configure the SoT modules.
In the case that the internal space is limited as in an automobile, sounds generated by placing the SoT module at various positions are audible to the listener as spatially balanced sounds rather than sounds spreading from one position. For example, sound can be generated at a small volume from the back portion of the front seat or behind the seat.
Not only for such acoustic applications, but also the SoT module can be used for a noise canceller in an automobile. Specifically, the SoT module is formed under the sheet, and the noise can be canceled with the sound in anti-phase to the engine sound.
If the above-described configuration would be realized with a speaker using a coil, it is difficult to secure the space in the automobile. Further, in terms of securing the power supply and reducing the weight, it is difficult to use a speaker using a coil. In contrast, as long as the SoT module using the piezoelectric element, a limited space, allowable weight and power source can be sufficiently utilized.
Electrical products are suitable for applications of SoT modules because power supply can be easily secured, and the housing can be utilized as a vibration plate. For example, the SoT module can be used for noise cancellation of a washing machine. In this case, the SoT module can be installed in the washing machine itself or can be installed in attachments of the washing machine. For example, it is preferable to install the SoT module on the pan of the washing machine as a noise canceller to form a mechanism that does not transmit sound. The sound leaked from the washing machine is a low sound of 1 kHz or less passing through the soundproofing material, and this sound can not be cancelled by the usual piezoelectric module, but it can be cancelled by the SoT module.
Typical applications of the SoT module comprise Cinematic Sound OLDE (CSO). CSO is a technique in which acoustic techniques are added to the self-emitting OLED to match the sound positions of the screens with the actual sound generating positions. With using an OLED panel as a vibration plate, the user can hear sound according to the image by directly transmitting sound from OLED screen, rather than from a separate speaker installed in the TV. That is, the user can hear the sound of talking with each other from the mouth of the performers of movies and dramas and can also hear the sound of the rain falling from the sky touching the ground from the position where the rain hits the ground on the actual screen. In this way, the user gets more immersion feeling. This application is not limited to TV, and the SoT module can be similarly applied to signage.
The SoT module is also applicable to furniture and architectural components. For example, the piezoelectric elements and the elastic bodies can be installed in the box-shaped drawer used in the rack frame are assembled to form a SoT module. In this way, the inside of the desk drawer can be sounded, and the inside of the box can be used as a speaker. Even if the drawer is filled with objects, a desired sound can be generated.
Piezoelectric elements and elastic bodies can also be installed on the iron plates behind LED projectors installed on roads, and iron plates can be used with vibration plates to configure SoT modules. An audible alarm can be generated directly from the LED projector, for example. It is also possible to configure a SoT module using a ceiling, wall or partition as a vibration plate. In that case, it can be used for both acoustic and noise cancellation. Such a configuration is also possible with a speaker by a coil in terms of sound pressure in the low audio frequency range, it is impossible to secure the space in the building. Further, a loudspeaker with a coil requires a strong power source, which may be subject to legal restrictions. SoT modules can be installed in small spaces, and they can be retrofitted by domestic power source for general use.
Formula (1) is a mathematical expression representing a natural frequency fs of a piezoelectric module. M and S represent the mass and stiffness of the piezoelectric module, respectively. In the case of a plate type piezoelectric module, the overall stiffness value mainly depends on the stiffness of the elastic body.
Therefore, by reducing the stiffness of the elastic body, the natural frequency of the entire system can be reduced. Further, since the stiffness of the entire system is also dependent on the tensile strength of the vibration plate, it is also possible to improve the sound pressure of low audio frequency sound according to the selection of the material of the vibration plate.
However, on the other hand, the transmissibility is lowered by the weight of the vibration plate, and there is also a possibility that the sound pressure characteristics deteriorate. In order to solve this problem, if the bonding strength between the piezoelectric composite and the vibration plate is increased to increase the transfer coefficient, the piezoelectric composite must receive all the weight of the panel, and the amplitude cannot be maintained. In consideration of such circumstances, sound pressure can be improved not only by adding an elastic body to the vibration path but also by adjusting the damping ratio of the vibration transmission path.
Piezoelectric modules for testing were prepared by varying the arrangement of elastic bodies, and the frequency characteristics of sound pressure were measured.
The piezoelectric module t2 for testing is configured of the piezoelectric element v1, the elastic bodies u2, the vibration plate w2. The two elastic bodies u2 respectively have the length of 8 mm in the longitudinal direction of the piezoelectric element v1 and is formed of urethane in the same manner as the elastic body u1, but they are respectively located at intermediate positions between the central portion and both end portions in the longitudinal direction of the element v1.
The piezoelectric module t3 for testing is configured of the piezoelectric element v1, the elastic bodies u3, the vibration plate w1. The two elastic bodies u3 respectively have the length of 8 mm in the longitudinal direction of the piezoelectric element v1 and is formed of urethane in the same manner as the elastic body u1, but they are respectively located at both ends in the longitudinal direction of the piezoelectric element v1.
The piezoelectric modules for testing were prepared by varying the shapes of the elastic bodies, and the frequency characteristics of sound pressure were measured.
As shown in
The frequency characteristics of the sound pressure was measured for SoT module 100 of the first embodiment (example E1 (parallel type)).
The SoT module 200 of the second embodiment (example E2 (end connection type)) was prepared to measure the frequency characteristics of the sound pressure.
The SoT module 700 of the seventh embodiment (example E7 (central connection loop type)) was prepared to measure the frequency characteristics of the sound pressure.
The SoT module 700 of the seventh embodiment (example E7 (central connection loop type)), the SoT module 800 of the eighth embodiment (example E8 (intermediate connection loop type)), and the SoT module 900 of the ninth embodiment (example E9 (end connection loop type)) were prepared, and the frequency characteristics of the respective sound pressures were measured.
The SoT module 1300 of the thirteenth embodiment (example E13 (single base plate type)) was prepared, the central piezoelectric element 1390 was driven in in-phase drive or anti-phase to the piezoelectric elements 1310 on both sides of the center, and frequency characteristics of the sound pressure were measured.
| Filing Document | Filing Date | Country | Kind |
|---|---|---|---|
| PCT/JP2021/041263 | 11/10/2021 | WO |
