Flat loudspeaker

Abstract

There is provided a flat loudspeaker comprising a housing in the form of a support frame, a sound-emitting rectangular membrane attached to the support frame, and an electrodynamic vibrator located on the opposite side of the sound-emitting rectangular membrane, to one end of which the vibrator is attached within a dedicated line that runs along the plane of the sound-emitting rectangular membrane, emerges from one of the vertices of the sound-emitting rectangular membrane, and terminates at a point on the opposite vertex of the horizontal surface of the sound-emitting rectangular membrane, located horizontally at a distance of two-thirds of the way from the top of the opposite side of the sound-emitting rectangular membrane.

Description

[Technical field]

[0001] The proposed technical solution is an acoustic wave generator that can also function as a broad spectrum flat panel loudspeaker. The proposed designed and manufactured flat panel loudspeaker is intended to bring quality advantages to the performance of an acoustic system. The flat loudspeaker is a flat panel acoustic system with a resonantly excited membrane that can be used to reproduce music and voice records in high quality. Many acoustic devices exist in the past, including cone speakers, dome speakers, and flat panel speakers. Such devices have several fundamental drawbacks. One of the most important drawbacks is the volume of air mass required for the operation of such acoustic devices. This drawback, in turn, leads to major drawbacks such as phase shift and mismatch, which are directly dependent on the frequency. [Background technology]

[0002] Since the speaker is a dipole transmitter, the positive phase in front of the speaker must match the negative phase behind the speaker.

[0003] This results in the use of precisely designed air-filled enclosures that reverse the phase from the rear of the speaker and add it to the front components. As a result, we have an audio system that is tuned to operate efficiently within a specific frequency in the acoustic range. Any deviation from the tuned frequency results in phase modulation, which causes parasitic harmonics, phase characteristic distortions in the audio recording and playback, as well as modulation that changes the amplitude frequency response of the audio signal.

[0004] There have been several attempts to create acoustic devices that do not have these drawbacks. Among them, flat-panel loudspeakers are based on the working principle of a resonating sound-emitting membrane and hold their own. Such acoustic devices do not require any enclosure and are characterized by a dipolar acoustic signal generation mode, i.e. essentially in phase in both directions from the membrane. Empirically, several design parameters have been established that directly affect the useful qualities of this type of acoustic device. These parameters are presented in Russian and international patents. Among them, the most important are design features such as the ratio of the membrane's width to its height, the mounting points of the acoustic exciter, the method of mounting the membrane, the type of actuator used, the design of the frame or enclosure, possible methods of matching the amplitude-frequency response of the acoustic system.

[0005] The techniques and methods recommended in various patents vary widely. When trying to put them into practical use, the inventors face many difficulties in ensuring the required sound quality. The fact that all the above-mentioned design features are closely related to each other is omitted. It is not possible to change one parameter without affecting the other parameter and then affect the other parameter, etc. In general, the design features described in many patents are more likely to be potentially possible than actually applicable, i.e., it all comes down to the possibility of trying different combinations and using different proportions, among which no one knows which will produce a useful sound effect, since it is entirely determined by rational practicality.

[0006] It is known that various sound emitting membrane designs are used for loudspeakers, for example, US Pat. No. 5,399,433 proposes using a plastic element of a tablet computer case as a sound emitting membrane.

[0007] Patent document 2 describes the properties of the membrane as well as the parameters influencing them (for example, honeycomb structures consisting of interlacing coverings of such panels, reinforcing fibres or spacers, and shells or sheets applied to the core of certain composite multilayer elements, contain particles in different orientations or relatively inclined on each face, i.e. in the form of several layers on each face), and envisages the use of membranes with honeycomb structures bent in space.

[0008] The '39 patent suggests using glass, wood or plastic as the membrane body, and the '40 patent suggests casting granular polystyrene as the membrane. All of these material parameters can strongly affect the physical properties of the membrane.

[0009] However, simply manufacturing a membrane from the above-mentioned materials, without taking into account the geometric parameters of the loudspeaker itself, does not improve the quality of the sound reproduction of the loudspeaker system.

[0010] The closest counterpart to the present invention is the device described in patent document 5, dated December 18, 2001, by Henry Azim. This patent describes an acoustic device that comprises a flat membrane, with at least one acoustic vibration driver, installed in the space opposite a dedicated part attached to the flat membrane, and operates on the principle of bending resonance mode. In addition, a preferred ratio for mounting the acoustic exciter within the panel area is also presented. Several values ​​are considered. For example, 24 possible combinations are considered from each corner, such as 3\7, 4\9, 5\13. That is, several positions for mounting the exciter are proposed. [Prior art documents] [Patent documents]

[0011] [Patent Document 1] WO 95 / 31805 [Patent Document 2] Russian Patent No. 2,692,096 [Patent Document 3] Russian Patent No. 2,427,100 [Patent Document 4] U.S. Pat. No. 3,779,336 [Patent Document 5] U.S. Patent No. 6,332,029 Summary of the Invention [Problem to be solved by the invention]

[0012] The inventors have found that using such percentages does not ensure the best possible quality of sound reproduction in an audio system. [Means for solving the problem]

[0013] The technical result is an improvement in the sound reproduction quality of the sound system.

[0014] This technical result is achieved by a flat loudspeaker comprising a housing in the form of a support frame, a sound-emitting rectangular membrane attached to the support frame, and at least one electrodynamic vibration exciter located on the opposite side of the sound-emitting rectangular membrane.

[0015] Furthermore, at one end of at least one of the vibrators, a sound-emitting rectangular membrane is attached within a dedicated line that runs along the plane of the sound-emitting rectangular membrane, emerges from one of the vertices of the sound-emitting rectangular membrane, and terminates at a point on the opposite vertex of the horizontal plane of the sound-emitting rectangular membrane, which is horizontally located at a distance of 2 / 3 from the top of the opposite surface of the sound-emitting rectangular membrane, and the sound-emitting rectangular membrane is fabricated as a surface layer that is bonded to both sides of the honeycomb filler and honeycomb structure, and a stabilizing impregnation liquid based on polyurethane primer and varnish covers the surface layer.

[0016] The layer of stabilizing impregnation solution based on polyurethane primer and varnish can be further coated with an acrylic polymer layer.Honeycomb fillers are made from materials consisting of paper, aramid fibers, aluminum, or other metals with low specific gravity.

[0017] Furthermore, the sound emitting rectangular membrane should preferably be characterized by a flange around its periphery.

[0018] If the stiffness of the membrane is uniform in different directions, the ratio of the long side to the short side of the membrane is 9 / 5. If the membrane stiffness is non-uniform in different directions and the ratio of the long side to the short side of the membrane is 9·k / 5, k is the ratio of the membrane stiffness in the long direction to the membrane stiffness in the short direction. Also, the sound emitting rectangular membrane needs to be attached to the supporting frame by foam tape placed around the sound emitting rectangular membrane. The invention is illustrated in the figures. [Brief description of the drawings]

[0019] [Figure 1] FIG. 1 demonstrates the proposed flat panel loudspeaker schematic. [Diagram 2] FIG. 1 demonstrates the main elements of the proposed flat panel loudspeaker. [Diagram 3] FIG. 1 demonstrates the main elements of the proposed flat panel loudspeaker. [Figure 4] FIG. 11 demonstrates the location of the dedicated (red) wire in the plane of the sound emitting membrane, where it is recommended to place at least one or more acoustic exciters. [Diagram 5] FIG. 13 is a diagram demonstrating the cross-sectional structure of the sound emitting membrane. [Explanation of symbols]

[0020] 1. Sound emitting membrane 2. Panel end edges made of plastic material 3. Foam tape to attach the membrane to the housing 4. Frame 5. Fixing strap 6, 6.1 to 6.5. Electrodynamic acoustic exciter 7. Amplifier connection terminal 8.Honeycomb filler 9.Coated paper 10. Impregnating fluid based on polyurethane primer and varnish 11. Acrylic Polymer DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

[0021] After much practical research, the inventors propose some technical solutions that have a direct positive impact on the creation of sound systems with good consumer characteristics, which are implemented in specific physical devices and methods for applying the technical solutions that aim to provide good sound effects.

[0022] The device consists of a support frame 4 (see FIG. 2), made of an inelastic plastic material capable of effectively absorbing vibration energy and which must be large enough to act as a fulcrum for bending the waves arriving from the exciter at the edge of the panel, and a membrane 1 intended to generate acoustic vibrations and transmit them to the air. On the surface of such a membrane, bands associated with different reproducible frequency ranges are modulated, but these bands themselves are distributed over the entire area of ​​the membrane. At least one or several electrodynamic exciters 6 are located opposite the membrane, at one end of which the membrane is attached in a dedicated line (see FIG. 4) running along the plane of the membrane. A flexible conductor, amplifier connection terminal 7 (see FIG. 2).

[0023] One of the important design parameters that determines the final sound quality of a flat panel loudspeaker system is the aspect ratio of the sound emitting membrane.

[0024] This is the ratio between the long side and the short side of the sound emitting membrane. The preferred aspect ratio of such membranes has been established by experiment and is at least 9 parts long side to 5 parts short side. Deviations in this ratio parameter may occur if the membrane stiffness is non-uniform in various directions. In such cases, the 9 / 5 aspect ratio must be adjusted by the k-factor, which defines the percentage difference between the membrane stiffness in the long direction and the membrane stiffness in the short direction. Thus, if the membrane stiffness is k percent higher in the long direction than in the short direction, the ratio is 9k\5.

[0025] Another important parameter when designing this type of loudspeaker system is the location of the exciters in the membrane area. For example, the aforementioned US Pat. No. 6,332,029 describes some preferred fixed ratios of acoustic exciters in the panel area. In this document, several values ​​are given. For example, 24 possible combinations are considered from each corner, such as 3\7, 4\9, 5\13, i.e. several positions for mounting the exciters are proposed.

[0026] The inventors found that using such a ratio does not ensure the maximum quality of sound reproduction of the acoustic system. As a result of numerous practical experiments, a dedicated EB line (see FIG. 4) running along the plane of the sound emitting membrane was established, within which the acoustic exciters, or several of them, must be installed so that the points of the rotation axis of the exciters cross the forward projection of the exciter circuit, which includes or is installed near the dedicated line. So, for a sound emitting membrane with an angle represented by points A, B, C, D, a dedicated "red" line of mounting of the exciters runs from point B to point E, which is the point of the DC side of the sound emitting membrane, by which the DC part is divided in the ratio DE\EC=1\2. Within the EB line, one or several exciters can be installed (see FIG. 6). For a technical solution with one acoustic exciter within such a line, it is necessary to determine the X point according to the ratio EB\XB=1.62. If several exciters are used within such a line, from point X, which defines the mounting point of the first exciter 6.1 (see FIG. 6), several exciters are fixed in the direction of point B, such that the distance between exciters 6.2, 6.3, 6.4 is as small as possible. It is also recommended to use an acoustic exciter designed to operate in the high frequency range, see 6.5 in FIG. 6. Such an exciter is fixed separately from the broadband signal exciter or exciters, but within a dedicated "red" EB line, preferably near corner B.

[0027] Of course, the red EB line can be reflected symmetrically along any of the film's axes of symmetry, so that its effect extends equally to the AF, DH, and CG lines (see Figure 4).

[0028] The advantage of the technical solution proposed in the form of a dedicated line within the membrane area, assuming that the excitation source is mounted within the membrane area, is that it has an excellent effect on the uniformity of the amplitude-frequency response by ensuring an optimal distribution of the resonant modulation within the membrane area, ensuring the naturalness of the sound, which is closely related to the total amount of distortion caused by the operation of the speaker system, reducing phase shifts, as well as ensuring the maximum frequency range when such a system is operated.

[0029] Another important parameter which directly ensures good acoustics is the membrane. After much practical research, an optimal design solution for a sound-emitting resonating membrane was identified (see Figure 5). Such a membrane consists of a honeycomb structure, a honeycomb filler 8, made of various materials such as paper, aramid fiber, aluminum, or another low-density metal. The membrane is accompanied by sheets of surface layers 9 bonded to both sides of the honeycomb structure by an adhesive composition capable of withstanding the bending vibrations caused by repeated vibrations.

[0030] As a covering material, it is proposed to use paper 9 with a density of 30-125 g per square meter of area. The covering paper 9 is then impregnated with a stabilizing impregnation liquid 10 based on polyurethane primer and varnish. Optionally, a layer of acrylic polymer 11 containing micron-scale crushed minerals and organic substances (quartz, walnut shells, rice and rice husks, etc.) is used. The layers 10 and 11 in Figure 5 mainly determine the elastic-plastic properties of the sound-emitting membrane, and the final tonal balance of the amplitude-frequency response,

[0031] The parameters that determine the reliability of the audio content reproduction are thus determined. The importance of reducing the final mass of the finished membrane as much as possible also became clear. This has a direct effect on the sensitivity of the loudspeaker system: the smaller the membrane mass, the higher the rate of rise of the pulse signal front, all other conditions being equal.

[0032] The actual density of the complete sound emitting membrane is in the range of 350-750g per square meter, which is a practical value. The membrane further includes an edge treatment that provides a semicircular sponge flange around the entire periphery of the membrane.

[0033] The flange is made of a material characterized by a relatively high (plastic) density and high value of plasticity, which allows a rapid damping of vibrations in relation to the thickness of such material. The flange 2 (see Fig. 2) serves to increase the mass of the membrane edge and to support a surface traveling wave propagating concentrically from the acoustic influence source towards the membrane edge, and to effectively reflect this wave in the opposite direction, ensuring a vibration mode in the modulation band of frequency-dependent amplitude bursts.

[0034] The internal structure of the honeycomb membrane can be 3-7 mm thick in practical applications. The parameters of thickness and stiffness need to be related to the actual size of the membrane. The actual size of the membrane with a specific stiffness is recommended based on the coefficients revealed by experimental studies.

[0035] In addition to the above technical solutions, it is necessary to mention the importance of the method of fastening the membrane to the frame of the acoustic device, which is a key parameter in determining the exact location of the amplitude modulation within the panel area, which in turn completely determines the acoustic characteristics of the flat loudspeaker.

[0036] The inventors have also identified a practically preferred method of mounting the membrane to the support frame, ensuring the best distribution of the zone of increasing vibration amplitude frequency modulation on the membrane's surface. This method is a semi-open mounting, where a foam tape is fixed to one side of the membrane along the entire circumference, most often with a gap of 10 mm between the membrane and the support frame. The foam tape holds the membrane edges to provide the necessary support mass (as well as edging the membrane edges with plastic material) as the interference from the primary surface traveling waves transforms, diverges from the acoustic excitation source, and processes it into secondary surface traveling waves, forming zones of increasing amplitude in the panel, which is key to the effective operation of the acoustic system itself. The semi-open mounting contributes to the effective performance of the foam rubber's other function of providing acoustic isolation between the membrane and the support frame, which dramatically affects the sound quality, reducing harmonic distortion in the acoustic signal generation process.

[0037] The proposed technical solution makes it possible to achieve a significant improvement in the quality characteristics of the loudspeaker system within one membrane with reduced labor and material costs, while at the same time allowing a significant increase in quality through the use of a minimum number of acoustic pathogens, saving costs and materials.

[0038] By applying the design method and technical solutions described in this patent, it is possible to create a wide-range loudspeaker system. This means in practice that a compact (flat) device is able to generate the entire spectrum of sounds audible to the human ear in the range of 20 Hz to 20,000 Hz. It can be argued that a practically superlative acoustic effect is achieved, while the degree of harmonic distortion is reduced to a minimum.

[0039] This is mainly due to the above mentioned technical solution designed to control the process of accurate distribution of frequency dependent burst bands of vibration amplitude over the area of ​​the sound emitting membrane. The accurate distribution of the burst bands is reflected in the frequency response graph as a line with minimal deviation from a straight line, which achieves useful acoustic effects such as a reduction in the "Doppler effect" of sound generation over a wide range. This harmful phenomenon is characterized by the fact that when different frequencies are generated simultaneously by one loudspeaker, distortions are generated for the listener due to the fact that the high amplitude low frequencies act as carriers for the low amplitude high frequencies. As a result, the high frequency components move towards and away from the listener, resulting in a "tremolo" effect as a distortion in the form of sound jitter.

Claims

1. A flat loudspeaker comprising a housing made as a support frame, a sound-emitting rectangular membrane attached to the support frame, and at least one electrodynamic vibration exciter located on the opposite side of the sound-emitting rectangular membrane, The sound-emitting rectangular membrane is attached to one end of at least one of the vibration exciters through a dedicated line; The dedicated line connects a start end on one side of the sound emitting rectangular membrane to a terminal end on the other side opposite to the one side of the sound emitting rectangular membrane along a plane of the sound emitting rectangular membrane, and the terminal end is located at a distance of 2 / 3 from an end of the other side on the other side, The sound-emitting rectangular membrane is prepared as a surface layer that is bonded to both sides of the honeycomb filler and honeycomb structure, and a stabilizing impregnation liquid based on polyurethane primer and varnish covers the surface layer; A flat loudspeaker, characterized in that the stiffness of the membrane is non-uniform in various directions and the ratio of the long side to the short side of the membrane is 9·k / 5, where k is the ratio of the stiffness of the membrane in the long direction to the stiffness of the membrane in the short direction.

2. 2. A flat loudspeaker according to claim 1, characterized in that the layer of stabilizing impregnation liquid based on polyurethane primer and varnish is further coated with a layer of acrylic polymer.

3. 2. The flat loudspeaker of claim 1, wherein the honeycomb filler is made of a material composed of paper, aramid fiber, aluminum, or other metals with low specific gravity.

4. 2. A flat loudspeaker as claimed in claim 1, characterized in that the sound emitting rectangular membrane has a flange around its periphery.

5. 2. A flat loudspeaker according to claim 1, characterized in that the sound-emitting rectangular membrane is attached to the support frame by a foam tape arranged around the periphery of the sound-emitting rectangular membrane.

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