The present disclosure is generally directed to multi-path acoustic waveguides.
In audio speakers, one factor that determines the sound quality is the sound pressure level (SPL), which generally depends in part on the speaker size relative to the distance between the speaker and the listener. Generally, a larger distance requires a larger speaker size. There is, however, a practical limit on the size of a large speaker. One solution is to use an array of smaller sized speakers to achieve similar acoustic results, because sound waves from the individual smaller speakers may combine to yield a combined sound wave that behaves similar to that emanating from a single large speaker. It is generally accepted that the spacing between two neighboring speakers needs to be smaller than the wavelength of the sound wave in question. The wavelength of a wave is determined as wave velocity divided by wave frequency. The wave velocity of sound in room temperature air is approximately 1130 ft/sec. For a low frequency audio sound having a frequency of 200 Hz, as an example, the corresponding wavelength is approximately 68 inches. Similarly, a midrange audio sound with a frequency of 2000 Hz, the corresponding wavelength is approximately 6.8 inches. A high frequency audio sound with an exemplary frequency of 20000 Hz has a wavelength is approximately 0.68 inches. It is difficult to achieve this small distance between speakers for high frequency sounds. This relatively small wavelength poses a problem for providing the desired spacing between high frequency speakers.
Acoustic waveguides have been developed to provide improved sound distribution from selected high-frequency drivers. Examples of such improved waveguides include the waveguides and associated technology set forth in U.S. Pat. Nos. 7,177,437, 7,953,238, 8,718,310, 8,824,717, and 9,204,212, and U.S. Patent Application Publication No. US2019-0215602, each of which is incorporated herein in its entirety by reference. While these waveguides provide substantial improvements particularly transmitting for high frequency audio sounds, there is still a need to distribute the emanation of the sound waves across the front of the speaker, producing a planar or cylindrical wavefront.
The technology disclosed herein relates to acoustic waveguides and associated systems. Several embodiments of the present technology are related to acoustic waveguides configured to be coupled to one or more selected high-frequency speaker drivers and that include sound channels configured to direct the sound waves produced by the speaker drivers through the sound channels and out of a front, distal end of the acoustic waveguide. Specific details of the present technology are described herein with respect to
The illustrated waveguide 100 includes a housing 103 having upper and lower housing portions 102 and 104 that can be coupled to a driver 101. In some embodiments, the housing portions 102 and 104 are mirror symmetrical about the mating plane of each housing portion 102 and 104 (such as the plane of the cross section of
As best seen in
As shown in
As seen in
In the illustrated embodiment, the housing portions 102 and 104 are configured to define eight sound channels 120a-h defining a path through the housing 103. In other embodiments, the housing 103 can have more or less than eight sound channels 120a-h, depending upon the desired configuration of the waveguide 100. In some embodiments, the sound channels 120a-h are configured so the ratio of the depth D of the waveguide 100 to the total width 108 of the outlet apertures 126a-h is in the range of about 1:1.2 to 1:2. In some embodiments the ratio is in the range of about 1:1.4 to 1:1.8. In the embodiment illustrated in
Referring again to
As shown in
After the sound waves from the driver enter the inlet aperture 116, the sound waves divide between inlet sound channels 117a and 117b, divide again between secondary sound channels 121ab, 121cd, 121ef, and 121gh, and finally divide into the sound channels 120a-h. The sound waves entering the waveguide 100 travel the same distance as each of the other sound waves in the other sound channels 120a-h and reach the outlet apertures 126a-h at the distal end 182 at substantially the same time. Based on the configuration of the inlet sound channels 117a and 117b, the secondary sound channels 121ab, 121cd, 121ef, and 121gh, and the sound channels 120a-h, each of the high-frequency sound signals entering the waveguide 100 at the same time will also exit the outlet apertures 126a-h at the same time, even though they each pass through different inlet sound channels 117a and 117b, secondary sound channels 121ab, 121cd, 121ef, and 121gh, and travel in different directions. In other embodiments, the individual sound channels 120a-h can be sized such that some or all of the corresponding sound paths 122a-h have different lengths. In some embodiments, the sound paths 122a-h have an acoustic length of between about 120% and 200% of the depth D (see
The secondary sound channels 121ab, 121cd, 121ef, and 121gh impart an initial arcuate bend to the sound paths 122a-h after the sound waves exit the inlet sound channels 117a and 117b. The initial arcuate bend directs the sound paths 112a-h laterally from a direction substantially perpendicular to the mounting flange 114. In this regard, the secondary sound channels 121ab, 121cd, 121ef, and 121gh change the direction of the sound waves by about 70° to about 90° from the direction at the inlet aperture 116. After the sound waves exit the secondary sound channels 121ab, 121cd, 121ef, and 121gh, the sound waves are divided into the sound channels 120a-h, which are each configured with various arcuate bends starting downstream of the secondary sound channels 121ab, 121cd, 121ef, and 121gh near the proximal end 180 of the housing portions 102 and 104. The bends in the sound channels 120a-h may be substantially smooth (i.e., not abrupt) as to not adversely interact with the sound waves traveling through the sound channels 120a-h. In some embodiments the radius of curvature of the bends in the sound channels 120a-h is equal to or greater than double the width of the sound channel.
In some embodiments, each of the sound channels 120a-h has a different arcuate bend based on the position of an outlet of the secondary sound channels 121ab, 121cd, 121ef, and 121gh and the outlet apertures 126a-h of each of the sound paths 122a-h. The waveguide 100 is generally mirror symmetrical about a plane parallel to the view in
In the illustrated embodiment shown in
The flaring of the one or more of the sound channels 120a-h can be achieved by a change in width of the sound channel along some or all of the sound channel, or by a change in height of the sound channel along some or all of the sound channel, or by a change in both the width and height of the sound channel along some or all of the sound channel. The lateral flare of the sound channels 120a-h includes lateral flare surfaces 132a-h and 134a-h, respectively, and creates a single, laterally united wavefront, as will be explained in greater detail below. The lateral flare surfaces of adjacent sound channels terminate at a peak, e.g., the lateral flare surface 132a and the lateral flare surface 134b terminate at a peak 124ab, the lateral flare surfaces 132b and 134c terminate at a peak 124bc, etc.
To ensure the sound waves spread laterally and combine sufficiently to form a united wavefront, the sound channels 120a-h (and 220a-f, and 250a-f for an acoustic waveguide 200, described below) may begin to flare in the lateral direction before reaching the distal end 182 (e.g., as shown in
The lateral flare surfaces 132a-h and 134a-h gradually flare and define a flare angle 146a-h at the distal portions of the sound channels 120a-h that can be between about and 25°, and more preferably in the range of about 10° and 20°. In other embodiments, the lateral flare surfaces 132a-h and 134a-h have a flare angle 146a-h at the distal portions of the sound channels 120a-h between about 12° and 18°. In further embodiments, the lateral flare surfaces 132a-h and 134a-h may have a flare angle 146a-h at the distal portions of the sound channels 120a-h between about 14° and 16°. The width of each outlet aperture 126a-h in the lateral direction can comprise between about 7% and 14% of the overall width 108 of the waveguide 100. In the illustrated embodiment, the width of each outlet aperture 126a-h in the lateral direction can comprise is about 8.33% of the overall width 108 of the waveguide 100. In other embodiments having between 12 and 8 sound channels, the width of each outlet aperture 126a-h in the lateral direction comprises between about 8% and 13% of the overall width 108 of the waveguide 100. Other embodiments having greater or fewer sound channels changes can have outlet apertures 126a-h with other widths in the lateral direction comprises relative to the overall width 108 of the waveguide 100.
It is noted that the sound channels 120 A-H have pipe resonance, were in the frequency of the pipe resonance depends on the length of the sound channel 120 A-H. The depth of the lateral flare surface is 132 A-H and 134A-H is determined by the overall depth D of the waveguide 100, and the depth of the flares generally controls how low in frequency the waveguide 100 can play. Accordingly, the dimensions of the sound channels 120 A-H, including the lengths of the portions of the sound channels, and the depth of the flares, are selected so that at least one of the pipe resonance frequency of the sound channel 120 A-H coincides with the low end of the waveguide designed frequency spectrum. As a result, the waveguide 100 is provided with a sensitivity boost at about the crossover frequency, which coupled with the sensitivity boost from the flared section, provides enhanced performance of the waveguide at and around the crossover frequency.
In embodiments with lateral flares, generally having lateral flare surfaces 132a-h and 134a-h, the depth of the flared portions of the sound channels 120a-h is between about 80% and 87% of the depth D of the waveguide 100, and/or the lateral flared portions of the sound channels 120a-h comprise between about 57% and 73% of the overall length of the sound paths 122a-h. In other embodiments, the depth of the flared portion of the sound channels 120a-h is between about 83% and 87% of the depth D of the waveguide 100, and/or lateral flared portions of the sound channels 120a-h comprise between about 60% and 64% of the overall length of the sound paths 122a-h. In at least one embodiment, the depth of the flared portion of the sound channels 120a-h is between about 84% and 86% of the depth D of the waveguide 100, and/or lateral flared portions of the sound channels 120a-h comprise between about 61% and 63% of the overall length of the sound paths 122a-h. In further embodiments, the depth of the flared portion of the sound channels 120a-h is greater than about 82% of the depth D of the waveguide 100, and/or the lateral flared portions of the sound channels 120a-h comprise about 65% of the overall length of the sound paths 122a-h. The lateral flare surfaces 132a-h and 134a-h may be defined by a conic shape having a fixed length, rho value, exit angle, entrance width, and exit width. In another embodiment with the sound channels 120a-h having different resonance frequencies than the above-referenced embodiment, the length of the sound channels 120a-h can be longer or have different lengths while having the lateral flare surface is 132a-h and 134a-h forming a percentage of the depth D of the waveguide 100. For example, the depth of the flared portion of the sound channels 100a-h can be in the range of approximately 55%-65%, or more specifically in the range of approximately 58%-62%, or more specifically, in the range of approximately 59%-61%, and even more specifically in the range of 59.62%-60.98%. In yet another embodiment wherein the sound channels 120a-h have different resonance frequencies than the above embodiments, the depth of the flared portion of the sound channels 120a-h can be in the range of approximately 49%-69%, or more specifically in the range of approximately 52%-66%, or more specifically, in the range of approximately 54%-64%, and even more specifically in the range of 54.67%-63.63%.
The vertical flare of the sound channels 120a-h includes vertical flare surfaces 136a-h and 138a-h, respectively, and creates radiation of the sound waves, to spread the sound waves vertically, such as the sound wave radiation from a horn, and to produce a substantially constant angle of radiation across a wide range of frequencies. In embodiments with vertical flares, generally having vertical flare surfaces 136a-h and 138a-h, the vertical flared portions of the sound channels 120a-h comprise between about 20% and 30% of the overall length of the sound paths 122a-h. In other embodiments, the vertical flared portions of the sound channels 120a-h comprise between about 23% and 27% of the overall length of the sound paths 122a-h. In further embodiments, the vertical flared portions of the sound channels 120a-h comprise about 25% of the overall length of the sound paths 122a-h. The vertical flare surfaces 136a-h and 138a-h may be defined by a dual conic shape having a first portion with a fixed length, rho value, exit angle, and exit width, and a second portion with a fixed length, rho value, exit angle, and exit width. The vertical flare surfaces 136a-h and 138a-h may be defined by other configurations, such as a conic-arc-conic configuration, or an arc-arc-conic configuration.
In some embodiments, the vertical flare surfaces 136a-h and 138a-h are configured to provide an acoustic dispersion pattern having an angle in the range of about 30°-130°. In the embodiment illustrated in
The flared shape described herein can be expected to maximize the efficiency with which sound waves traveling through the sound channels 120a-h are transferred into the air outside of the housing portions 102 and 104. The flaring may also help damp pipe resonances that may exist within the sound channels 120a-h, such as by adding an exponential curve to the flared surfaces. In other embodiments, however, the sound channels 120a-h may not have a flared configuration, or the amount of flaring occurring in some or all of the sound channels may be different. In other embodiments, the sound channels 120a-h can be further divided, such as by providing shaped inserts or dividing structures (not shown) that split the sound channels 120a-h into two or more subchannels, each of which has the same overall sound path length as the other sound channels 120a-h.
Adjustments to the dimensions of the sound channel can also be achieved by controlling the channel height along some or all of the length of the channel. For example,
In this illustrated embodiment, each sound channel 120a-h can flare vertically as it approaches the distal end 182 of the housing portions 102 and 104, such that the channel has a first height H1 (
The distal end 182 may be generally perpendicular to the longitudinal axis of the waveguide 100 when viewed from the side, such as in the orientation shown in
Among other differing aspects, the acoustic waveguide 200 differs from the waveguide 100 by having separate but mirror symmetrical sound channels relative to each high-frequency driver HFD. In this regard, a plurality of sound channels 220a-f, extending from the inlet aperture 216a, are mirror symmetrical to a plurality of sound channels 250a-f, extending from the inlet aperture 216b, about a centered vertical, longitudinal plane parallel to the orientation and located equidistant between the inlet apertures 216a and 216b. While the same mirror symmetry of the housing 203 about the mounting surfaces is present, the mirror symmetry about the vertical, longitudinal plane provides an increased soundstage at the outlet apertures 226a-f and 256a-f. Unlike the waveguide 100, in the acoustic waveguide 200, each separate mirror symmetrical sound channel group (e.g., 220a-f or 250a-f) is not itself mirror symmetrical about a central axis of the respective inlet aperture 216a and 216b. For example, while the outermost sound channels 120a and 120h of the waveguide 100 are mirror symmetrical about the central axis of the inlet aperture 116, the outermost sound channels 220a and 220f (or 250a and 250f) are not mirror symmetrical about the central axis of the inlet aperture 216a (or 216b).
In the illustrated embodiment, each group of sound channels 220a-f and 250a-f has six channels. In other embodiments, each group has greater than four sound channels. The acoustic waveguide 200 may also omit the inlet sound channels (i.e., the inlet sound channels 117a and 117b of the waveguide 100) and transition the sound waves directly to secondary sound channels 221ab, 221cd, 221ef, 251ab, 251cd, and 251ef, among other possible configurations. The sound channels 220a-f and 250a-f may include a fewer or greater quantity or degree of arcuate bends when compared with the sound channels 120a-h, such as shown in
The acoustic waveguide 200 includes two sets of high-frequency sound channels 220a-f and 250a-f, each coupled a respective one of the two drivers 201. As described above with respect to the waveguide 100, the sound channels 220a-f and 250a-f terminate at outlet apertures 226a-f and 256a-f in the distal end 282 of the housing 203. In the illustrated embodiment, a distal mounting flange 210 is provided at the distal end 282 of the housing 203 generally adjacent to the outlet apertures 226a-f and 256a-f. The distal mounting flange 210 may be configured to be affixed to a speaker housing (not shown) to hold the acoustic waveguide 200 and the associated high-range drivers 201 in position in the speaker housing. In some embodiments, the mounting flange 210 can be used to couple the acoustic waveguide 200 to a horn (not shown), such as a horn attached to the speaker housing.
In some embodiments, the lateral flare surfaces 232a-f, 234a-f, 262a-f, and 264a-f may have flare angles 246a-f and 286a-f between about 10° and 20°. In other embodiments, the lateral flare surfaces 232a-f, 234a-f, 262a-f, and 264a-f may have flare angles 246a-f and 286a-f between about 14° and 18°. In further embodiments, the lateral flare surfaces 232a-f, 234a-f, 262a-f, and 264a-f may have flare angles 246a-f and 286a-f of about 16°. The width of each outlet aperture 226a-f and 256a-f in the lateral direction can comprise between about 7% and 14% of the overall width 209 of the acoustic waveguide 200. In other embodiments, the width of each outlet aperture 226a-f and 256a-f in the lateral direction comprises between about 8% and 13% of the overall width 209 of the acoustic waveguide 200.
In embodiments with lateral flares, generally having lateral flare surfaces 232a-f, 234a-f, 262a-f, and 264a-f, the depth of the flared portions of the sound channels 220a-f and 250a-f is between about 80% and 87% of the depth D of the acoustic waveguide 200, and/or the lateral flared portions of the sound channels 220a-f and 250a-f comprise between about 57% and 73% of the overall length of the sound paths 222a-f and 252a-f. In other embodiments, the depth of the flared portion of the sound channels 220a-f and 250a-f is between about 83% and 85% of the depth D of the acoustic waveguide 200, and/or lateral flared portions of the sound channels 220a-f and 250a-f comprise between about 62% and 68% of the overall length of the sound paths 222a-f and 252a-f. In further embodiments, the depth of the flared portion of the sound channels 220a-f and 250a-f is greater than about 82% of the depth D of the acoustic waveguide 200, and/or the lateral flared portions of the sound channels 220a-f and 250a-f comprise about 65% of the overall length of the sound paths 222a-f and 252a-f. The lateral flare surfaces 232a-f, 234a-f, 262a-f, and 264a-f may be defined by a conic shape having a fixed length, rho value, exit angle, and exit width. In yet another embodiment wherein the sound channels 220a-f and 250a-f have different resonance frequencies than the above embodiments, the depth of the flared portions of the sound channels 220a-h and 250a-f having lateral flare surfaces 232a-f, 234a-f, 262a-f, and 264a-f can be in the range of approximately 65%-78%, or more specifically in the range of approximately 68%-75%, or more specifically, in the range of approximately 70%-73%, and even more specifically in the range of 70.73%-72.99%.
In embodiments with vertical flares, generally having vertical flare surfaces 236a-f, 238a-f, 266a-f, and 268a-f, the vertical flared portions of the sound channels 220a-f and 250a-f comprise between about 20% and 30% of the overall length of the sound paths 222a-f and 252a-f. In other embodiments, the vertical flared portions of the sound channels 220a-f and 250a-f comprise between about 23% and 27% of the overall length of the sound paths 222a-f and 252a-f. In further embodiments, the vertical flared portions of the sound channels 220a-f and 250a-f comprise about 25% of the overall length of the sound paths 222a-f and 252a-f. The vertical flare surfaces 236a-f, 238a-f, 266a-f, and 268a-f may be defined by a dual conic shape having a first portion with a fixed length, rho value, exit angle, and exit width, and a second portion with a fixed length, rho value, exit angle, and exit width. In some embodiments, the vertical flare surfaces 236a-f, 238a-f, 266a-f and 268a-f are configured to provide an acoustic dispersion pattern having an angle of about 90° from the distal end 282 along the vertical direction.
In some embodiments, the sound paths 222a-f and 252a-f have an acoustic length of between about 120% and 200% of the depth D (see
As used in the foregoing description, the terms “vertical,” “lateral,” “upper,” and “lower” can refer to relative directions or positions of features in the waveguide in view of the orientation shown in the Figures. For example, “upper” or “uppermost” can refer to a feature positioned closer to the top of a page than another feature. These terms, however, should be construed broadly to include waveguides having other orientations, such as inverted or inclined orientations where top/bottom, over/under, above/below, up/down, left/right, and distal/proximate can be interchanged depending on the orientation. Moreover, for ease of reference, identical reference numbers are used to identify similar or analogous components or features throughout this disclosure, but the use of the same reference number does not imply that the features should be construed to be identical. Indeed, in many examples described herein, identically numbered features have a plurality of embodiments that are distinct in structure and/or function from each other. Furthermore, the same shading may be used to indicate materials in cross section that can be compositionally similar, but the use of the same shading does not imply that the materials should be construed to be identical unless specifically noted herein.
The foregoing disclosure may also reference quantities and numbers. Unless specifically stated, such quantities and numbers are not to be considered restrictive, but exemplary of the possible quantities or numbers associated with the new technology. Also, in this regard, the present disclosure may use the term “plurality” to reference a quantity or number. In this regard, the term “plurality” is meant to be any number that is more than one, for example, two, three, four, five, etc. For the purposes of the present disclosure, the phrase “at least one of A, B, and C,” for example, means (A), (B), (C), (A and B), (A and C), (B and C), or (A, B, and C), including all further possible permutations when greater than three elements are listed.
From the foregoing, it will be appreciated that specific embodiments of the new technology have been described herein for purposes of illustration, but that various modifications may be made without deviating from the present disclosure. Accordingly, the invention is not limited except as by the appended claims. Furthermore, certain aspects of the new technology described in the context of particular embodiments may also be combined or eliminated in other embodiments. Moreover, although advantages associated with certain embodiments of the new technology have been described in the context of those embodiments, other embodiments may also exhibit such advantages and not all embodiments need necessarily exhibit such advantages to fall within the scope of the present disclosure. Accordingly, the present disclosure and associated technology can encompass other embodiments not expressly shown or described herein.
This application is a continuation of U.S. patent application Ser. No. 17/212,510, filed Mar. 25, 2021, which claims priority to and the benefit of U.S. Provisional Application No. 62/994,754, filed Mar. 25, 2020, both of which are incorporated herein by reference in its entirety.
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Parent | 17990087 | Nov 2022 | US |
Child | 18344797 | US | |
Parent | 17212510 | Mar 2021 | US |
Child | 17990087 | US |