1. Field of the Invention
This invention relates broadly to audio speaker systems. More particularly, this invention relates to horn-type audio speaker systems.
2. State of the Art
Loudspeaker systems typically employ one or more of the following speaker elements: i) a sub-woofer that reproduces extremely low frequencies from about 20 Hz to 100 Hz; ii) a woofer that reproduces low frequencies from about 100 Hz to 500 Hz; iii) a mid-range speaker that reproduces frequencies from about 500 Hz to 6 kHz; and iv) a tweeter that reproduces high frequencies from about 6 kHz to 11-12 kHz (and possibly to 20 kHz). In such systems, cross-over circuitry delivers the appropriate frequency range to the separate speakers. There are two ways that the cross-over circuitry can be connected to the speaker system. In low and medium power applications, the cross-over circuitry is connected after the amplifier. In such configurations, the cross-over circuitry is typically disposed within the speaker cabinet. For high power applications, the cross-over circuitry is connected before the amplifier.
Sub-woofers, woofers and mid-range speakers typically emit sound in a highly dispersed manner. In contrast, tweeters typically emit sound in a highly directional manner. Thus, the dispersion pattern of the tweeter (which is the extent to which the tweeter yields acoustic radiation over a given area) is of particular importance in designing a speaker which has wider dispersion overall. There are several different types of tweeters including cone tweeters, dome tweeters, and horn tweeters.
Cone tweeters utilize a shallow cone surface with a sound producing diagram at its apex. Cone tweeters are efficient and most economical, and typically provide a narrow dispersion pattern.
Dome tweeters utilize a dome diaphragm to produce sound. The dome diaphragm is typically made of light hard metal (such as titanium), rigid plastic compounds, or soft silk-like material. Dome tweeters are efficient, yet typically provide narrow dispersion patterns for frequency components above 10 kHz.
Horn tweeters utilize a horn surface (which is typically curvilinear or exponential in nature) with a relatively small sound-producing element at its apex. Typically, horn tweeters are designed to provide a narrow dispersion pattern with a dispersion angle between 60 and 90 degrees for the high frequency audio signal components supplied thereto by the crossover-circuitry.
A wide dispersion pattern is desirable in some acoustic applications, such as distributed audio installations that require many loudspeakers for the desired acoustic coverage of the listening space. In such applications, the wide dispersion pattern reduces the number of speakers required to cover the listening area, and thus reduces costs. As described above, conventional tweeter designs are limited in their dispersion pattern (generally less than 90 degrees) for high frequency audio signal components, and thus are unsuitable for use in these applications. Thus, there remains a need in the art to provide audio speaker components that have wide angle dispersion characteristics for high frequency signal components and thus are suitable for use in acoustic applications requiring wide coverage such as distributed audio installations.
Moreover, it is desirous in many of these applications that the speaker components reproduce frequencies generally supported by a mid-range speaker (typically below 6 kHz down to 500 Hz). This extended frequency range also reduces the number of speakers required to cover the listening area and reduces costs. As described above, conventional tweeter designs support only high frequency components and thus fail to provide the benefits of an extended frequency range. Therefore, there remains a need in the art to provide audio speaker components that have wide angle dispersion characteristics over an extended frequency range.
Finally, it is desirous in many of these applications that the speaker provide a uniform dispersion pattern (typically referred to as “constant beamwidth” or “constant directivity”) with respect to the area covered by the speaker. This feature simplifies the layout and design of the loudspeakers of the system in order to provide uniform coverage over the intended listening area. However, typical “constant beamwidth” horn tweeters are limited in their dispersion pattern (generally less than 90 degrees), and thus are disadvantageous in these applications. Therefore, there remains a need in the art to provide audio speaker elements that have uniform dispersion characteristics suitable for such wide coverage acoustic applications.
It is therefore an object of the invention to provide an audio speaker system which has a wide dispersion pattern for high frequency sound components.
It is another object of the invention to provide an audio speaker system which has a wide dispersion pattern for a broad frequency spectrum of sound.
It is a further object of the invention to an audio speaker system which has a uniform dispersion pattern for a broad frequency spectrum of sound.
In accord with these objects which will be discussed in detail below, the audio speaker system of the present invention includes a speaker driver operably coupled to a horn waveguide. The speaker driver reproduces sound within an extended frequency range that includes a high frequency band between 8 kHz and 11 kHz. In the preferred embodiment, the extended frequency range includes a wide frequency band between 2 kHz and 11 kHz (and most preferably includes the ultra-wide frequency band between 800 Hz and 11 kHz). The horn waveguide has an axi-symmetrical waveguide surface that provides for uniform polar dispersion at dispersion angles greater than 90 degrees for sound within the extended frequency range. The waveguide surface preferably has an annular cross section with a radial dimension that increases curvilinearly from its throat to its mouth.
According to one embodiment, the waveguide surface of the horn is a tractroid surface.
According to another embodiment, the waveguide surface of the horn is exponential in nature.
According to a preferred embodiment of the invention, the critical parameters of the horn (throat area, mouth area, length) are adapted to provide a frequency response which encompasses a substantial part of the extended frequency range supported by the speaker driver.
In another aspect of the present invention, an audio speaker system employs an annular gasket that separates the sound reproducing membrane of a speaker driver with a horn waveguide. The annular gasket is disposed in an area outside of and adjacent to the throat of the horn waveguide. The annular gasket is preferably realized from closed cell foam or other compliant acoustically-absorbable material. The gasket minimizes the volume of the compression chamber that the sound reproducing membrane is compressing, thus leading to less frequency cancellation (which leads to improved frequency response of the speaker driver).
Additional objects and advantages of the invention will become apparent to those skilled in the art upon reference to the detailed description taken in conjunction with the provided figures.
Turning now to
The speaker driver 12 is preferably a high fidelity speaker driver providing a 13 relatively flat response (e.g., ±3 dB) throughout a relatively large frequency range (for example, between 800 Hz and 15 kHz). Cross-over filter circuitry 20, which is preferably integral to the enclosure 11, is operably coupled between an audio signal source (e.g., amplifier) and the speaker driver 12. Preferably, the cross-over filter circuitry 20 provides a high pass filter with a cut-off frequency that matches the lower end of the frequency range (for example, 800 Hz) supported by the speaker driver 12.
The horn 14 (or a portion thereof) defines a waveguide surface having an annular cross-section with a radial dimension that increases curvilinearly from the throat 16 to the mouth 18 as shown in
x=sech(u)×cos(v)
y=sech(u)×sin(v)
z=(u)−tan h(u)
where the z-axis corresponds to the central axis, and the x and y axes are orthogonal to the z-axis as shown.
Alternatively, the waveguide surface of the horn 14 may be “exponential” in nature (i.e., where the horn length is exponentially related to the area of the horn mouth) or any other curvilinear surface with a smooth flare rate. The expression for such an “exponential” waveguide surface is S=S1emx, where ‘S’ is the area of the horn mouth, ‘S1° is the area of the horn throat, ‘m’ is the flare constant of the horn waveguide surface, and ‘x’ is the length of the horn waveguide surface.
The frequency response (e.g., the low cutoff frequency and high cutoff frequency) of the horn 14 is dependent upon the area of the throat 16 (which is governed by the diameter of the throat DT), the area of the mouth 18 (which is governed by the diameter of the mouth DM), and the length L of the horn as well as other parameters as is well known in the audio speaker arts. In the preferred embodiment of the present invention, these parameters are adapted to provide a frequency response between 800 Hz and 11 kHz, which encompasses a substantial part of the frequency range between 800 Hz and 15 kHz supported by the speaker driver 12.
The sound waves produced by the speaker driver 12 are emitted from the horn 14 in a dispersion pattern that is characterized by a dispersion angle, which is the angle at which the sound level is reduced by 6 dB as compared to the on-axis sound level. An array of dispersion angles are shown in
x=sech(u)×cos(v)
y=sech(u)×sin(v)
z=(u)−tan h(u)
where the z-axis corresponds to the central axis, and the x and y axes are orthogonal to the z-axis as shown.
The dimensions of the horn (which are shown in
The waveguide surface 22′ of the horn 14′ provides uniform polar dispersion of sound at wide dispersion angles over an extended frequency range between 800 Hz and 11 kHz as described above with respect to the beamwidth curve of
Different views of a solid model of the horn 14′ are shown in
In the preferred embodiment, the speaker driver 12 is rear-vented to enable low frequency components to be emitted from the backside of the speaker driver 12 into a rear chamber 26 as shown in
The horn-loaded speaker device of
As shown in the cross-section of
There have been described and illustrated herein several embodiments horn-loaded audio speaker systems that provide improved frequency response (and more particularly wide dispersion characteristics over an extended frequency range). While particular embodiments of the invention have been described, it is not intended that the invention be limited thereto, as it is intended that the invention be as broad in scope as the art will allow and that the specification be read likewise. Thus, while particular sizes, shapes and materials have been disclosed for various components of the horn-loaded speaker system, it will be appreciated that other sizes, shapes and materials can be used as well. In addition, while particular types of waveguide surfaces (e.g., exponential and tractroid) have been disclosed, it will be understood that other forms of axi-symmetrical surfaces can be used. Moreover, the omnidirectional wide dispersion angle characteristics of the horn-loaded speaker device may be adapted to extend (or to shorten) the top end of the frequency range (e.g., between 1 kHz and 11 kHz) described herein up to 20 kHz. Similarly, the omnidirectional wide dispersion angle characteristics of the horn-loaded speaker device may be adapted to extend (or to shorten) the bottom end of the frequency range (e.g., between 1 kHz and 11 kHz) described herein. It will therefore be appreciated by those skilled in the art that yet other modifications could be made to the provided invention without deviating from its spirit and scope as claimed.