JBL Technical Note - Vol.1, No.35 电路原理图.pdf
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1、 1 Technical Notes Volume 1, Number 35 CBT Constant Beamwidth TechnologyTM Introduction Column loudspeakers have become an important form factor for loudspeakers throughout the years. The tall and slender package fits nicely into a wide variety of architectural styles, and the columns provided perfo
2、rmance characteristics that work nicely for certain application and room types. Recently, column speakers have become more popular than ever, and an even more important element in the sound designers toolbox for aesthetic reasons and the natural narrow vertical coverage. Large format line arrays hav
3、e become increasingly common for large- scale sound reinforcement, and columns are a logical step-down in size from such line arrays. DSP technology and control interfaces have advanced to the point where powered column speakers having individual DSP processing for each driver and real-time remote c
4、ontrol over the entire system is becoming economically feasible but still expensive. In addition, an appreciation of the importance of pattern control is expanding in the audio design community. This paper explains JBLs Constant Beamwidth TechnologyTM, which has been implemented in the CBT Series of
5、 non-powered line array column loudspeakers. These speakers solve many of the problems associated with traditional passive column speakers, as well as some issues present in powered columns, and in point-and-shoot loudspeakers. The end result is a line of affordable passive column speakers that prov
6、ides constant directivity within narrow vertical coverage angles. They provide consistent frequency response regardless of distance or off-axis location within the listening zone, suppression of side lobes, switchable vertical coverage, asymmetrical vertical coverage for more uniform sound levels wi
7、th in the room from front-to-back, and are practical for a wide variety of sound reinforcement projects. 2 History The use of an array of loudspeakers to increase directivity can be dated back to the early era of public address systems in the 1930s. Increased directivity has long been known to impro
8、ve intelligibility of sound systems. In the late 1950s and early 1960s there was an explosion in the use of column line arrays1,2,3. Designers sought to control the directivity with configuration and filtering techniques on line arrays of multiple transducers. The traditional thinking was that the d
9、irectivity is directly related to the size of the array. Therefore to keep the directivity constant the effective size of the array would need to change with frequency. In the early 1970s the first true constant directivity devices in the form of horns were introduced. While a great leap forward for
10、 point and shoot systems they yielded less than ideal coverage when used as components in large arrays and were limited in bandwidth. Early examples from Klepper and Steele1 and Novak2 show novel approaches for the time that include frequency tapering of the line and amplitude shading. The frequency
11、 shading attempts to use the outermost drivers to control directivity at the lowest frequencies and then moves the sound sources toward the center of the array as the response rises by low pass filtering the outer elements. This makes the apparent aperture or source size decrease with frequency whic
12、h keeps the beam relatively constant in width with frequency. The authors of the early works acknowledged that the concept is challenged by the phase response of the filters which results in the sources not operating in phase at all frequencies, as would be desired, limiting the performance of the m
13、ethod. The idea is to make the effective size of the array a fixed ratio of the wavelength that it is producing. Figure 1. From Klepper and Steele1 shows a simple network for improving directivity control and Novak2 (on the right) shows more complex filtering 3 Klepper and Steele1 also show the valu
14、e of amplitude shading (reducing the output at the ends of the array) in improving dispersion and reducing side lobes. Figure 2. From Klepper and Steele1, a novel passive approach to amplitude shading a line array with an absorbing medium. In the 1980s, as designers began to use computers and imagin
15、e the use of digital delay for beamforming, further refinement of line array beamwidth control was demonstrated. Augspurger and Brawley4 showed the computer modeling of a line array with delay and the use of a Bessel function for the amplitude shading. Figure 3. From Augspurger and Brawley4 showing
16、that relatively even coverage off axis can be obtained with delay and that with the addition of Bessel shading very smooth off axis behavior can be obtained. 4 While the simulation does not show constant directivity (which would yield flat parallel off axis curves) the paper shows that delay arcing
17、of the speakers and Bessel amplitude shading provides a very useful solution. This approach would pave the way for the CBT concept. Many analog approaches have been implemented over the years with limitations in performance. In recent years the method was improved upon by using zero phase shift digi
18、tal FIR filters by Horbach and Keele5. They outline the expected performance of a log (driver spaced) array with new DSP filtering techniques. The system is very effective in controlling beamwidth. However this approach, like the earlier system, suffers from limited maximum high frequency output bec
19、ause the last octave is only being covered with two small drivers. Figure 4. Figures (15, 16, 17) from Horbach and Keele5, log array with zero phase shift Finite Impulse Response filters to achieve constant directivity. Straight line arrays without any frequency shading or amplitude shading have fou
20、nd favor in the marketplace for some time. The property that is most often claimed is that they create cylindrical waves. While a line source of infinite length will create cylindrical waves, finite size arrays only create wave fronts resembling cylindrical waves over a narrow region in space and fr
21、equency. The region is defined by the height of the array. Simple superposition models of straight line arrays with discrete radiation elements work quite well to show the actual behavior of real finite line arrays. While purporting to create a wedge of sound the array has a pattern than narrows con
22、stantly with frequency and is uneven. Additionally, the response changes with distance 5 Normalized off axis frequency Response of 16 driver 1m array flat at 25 feet on axis -30 -20 -10 0 10 10010000 Freq dB 2 4 6 Off axis response at 25 ft 2, 4 and 6 degrees off axis. Response changes radically wit
23、hin a very small forward beam. Normalized on axis frequency Response of 16 driver 1m array flat at 25 feet, versus distance -30 -20 -10 0 10 10010000 Freq dB 6 12 50 Figure 5. The simulated on and off axis behavior of a finite straight line array of 16 elements 1m tall and the response at 6, 12 and
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