JBL Technical Note - Vol.1, No.30 电路原理图.pdf

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1、1 Technical Notes Volume 1, Number 30 Cone Midrange Compression Drivers (CMCD) Introduction: Throughout the history of professional audio it has been realized there are distinct performance advan- tages to compression and horn-loading a midrange transducer. The advantages include increased sensitivi

2、ty and bandwidth, desirable pattern control, and arrayability - all provided by horn-loading. Other advantages include reduced harmonic and inter- modulation distortion, and increased maximum SPL. Unfortunately, these theoretical benefits have been difficult to simultaneously achieve in practice, du

3、e to the lack of transducers that are suited to this appli- cation, but also due to compromises in the design of the horn and/or phasing plug. Because of these limitations, many previous solu- tions have suffered from poor frequency response, restricted high frequency bandwidth, and non-ideal area e

4、xpansions that introduce other anomalies. These limitations, and others, contribute to audible irregularities often referred to as a “horn midrange sound”. This technical note will discuss how these limitations were overcome in the family of JBL Cone Midrange Compression Drivers (CMCDs). Pertinent p

5、erfor- mance figures are presented in comparison and in contrast to other past and present solutions. Finally, typical CMCD performance characteristics are provided. Historical and Technical Background: The design of horn-loaded midrange systems can broadly be categorized into two philosophies: The

6、first is based on high-frequency compression driver designs that are optimized to operate over a lower frequency range. The second approach uses a cone midrange loaded directly by the horn, or coupled to the horn with a phase plug. Solutions derived from a high frequency compres- sion driver may hav

7、e numerous problems, includ- ing high harmonic distortion (due to high compres- sion ratios, and limited excursion capability), and limited low frequency extension (due to improper Theil-Small parameters for this application). These designs may break under high output, or inadvert- ent abuse. They r

8、equire a very large horn in order to operate optimally. The second solution a cone midrange driver coupled to a horn can correct most of the problems of a compression horn-loaded midrange system. However, other limitations are often introduced. One of these limitations in the past has been limited h

9、igh-frequency extension. Even an ideal cone transducer has a mass break point of ap- proximately 600 Hz to 900 Hz which limits high frequency extension. While many manufacturers attempt to correct this with various phase plug designs, the limitation still exists the moving 2 mass is too high, and th

10、e motor force provided by the magnet structure limits sensitivity. As well, many phase plug and displacement plug designs do not provide the uniform compression of the wavefront required to produce extended and smooth frequency response. After evaluating the state-of-the-art, JBL engineers developed

11、 a new family of midrange devices that eliminate performance limitations, and maximize sound quality. The resulting midrange components are referred to as a Cone Midrange Compression Driver (CMCD). These proprietary JBL implemen- tations are patent-pending. CMCD models are based around industry ac-

12、cepted, and proven, high-output JBL midrange transducers such as the 2250, used in VERTEC VT4889 line-array systems, and the 165H, used in Cinema ScreenArray systems. These transducers meet and achieve the requirements for optimal performance in a CMCD configuration. Key Performance Features: CMCD m

13、odels include the CMCD-81J, CMCD- 81H, and the CMCD-61H. Each CMCD assembly incorporates a JBL cone midrange driver, a 3 slot annular-ring phasing plug, and a thermally conduc- tive rear chamber. An optimal 4-inch exit-diameter and a correct exponential expansion provide excellent coupling to the en

14、tire family of Progres- sive TransitionTM midrange waveg uides. Section- views of the CMCD-81H/J, and CMCD61H, coupled to a PT waveguide, are shown in Figures 1 and 2. CMCD-81 models have a recommend bandwidth of 250 Hz to 2.0 kHz, and power handling of 350 watts. Sensitivity is 107 dB SPL/1w/1m on

15、a typical 90 x50 waveguide. Frequency response and electrical impedance are shown in Figure 3. Due to pistonic response within the pass-band, re- sponse deviations of less than 0.5 dB result with simple equalization. Maximum continuous SPL exceeds 133 dB SPL at 1 meter on appropriate waveguides. The

16、 CMCD-61H recommended bandwidth is 400 Hz to 3.5 kHz. Power handling is 125 watts. Sensitivity at 1 watt/1 meter is 107 dB SPL on a typical 90 x50 waveguide. Frequency response and electrical impedance are shown in Figure 4. Due to pistonic behavior throughout the pass-band, response variations of 0

17、.5 dB are realized with simple EQ. Maximum SPL exceeds 128 dB at 1 meter. The CMCD-81 is ideally suited for applications that call for maximum output, or where a lower cross- over to the low-frequency section is required. The CMCD-61 is suited to applications where extreme SPL is not required. In in

18、stallations where cost is critical but pattern control, low distortion, and excellent midrange clarity are still required, systems incorporating a CMCD-61H are an ideal solution. Figure 1:Section View of CMCD-81H and PT Midrange Waveguide. Figure 2:Section View of CMCD-61H and PT Midrange Waveguide.

19、 3 100100010000 70 80 90 100 110 Impedance (ohms) 10 100 2020K dB SPL Frequency (Hz) 1 Watt Sensitivity and Impedance 100100010000 70 80 90 100 110 Impedance (ohms) 10 100 2020K dB SPL Frequency (Hz) 1 Watt Sensitivity and Impedance Figure 4: Frequency Response and Impedance of CMCD-61H with 90 x 50

20、 PT Waveguide. Figure 3: Frequency Response and Impedance of CMCD-81H with 90 x 50 PT Waveguide. 4 Technical Details: CMCD assemblies use 8-inch and 6.5-inch cone midrange drivers designed from the ground-up to operate as true compression loaded midrange devices. The phasing plugs, and optimal rear

21、chambers, provide maximum sensitivity and wide bandwidth. Design features for improved performance include: Small diameter midrange cone drivers, thermally conductive rear enclosures, and annular ring phase plugs with 4-inch exit diameters. The benefit of each feature is elaborated on in the followi

22、ng sections: True Annular Ring Phasing Plug: CMCD designs feature a three-slot annular-ring phasing plug to provide optimal loading of the cone diaphragm to frequencies as high as 3.5 kHz in the case of the CMCD-61H. CMCD assemblies employ phasing-plugs die-cast in a high-density polyester-fiberglas

23、s thermoset- composite. The phase plugs are rigidly-bounded three-piece annular designs. This construction allows for close dimensional tolerances in produc- tion, and eliminates variability. CMCD phase plugs are typically spaced 0.075 inches from the cone. Many solutions have incorporated either on

24、e-piece displacement plugs, or molded polystyrene foam phase plugs. In either case the results are not optimal due to acoustical losses in the phase plug, and excessive spacing from the speaker cone. Sensitivity and high frequency extension are compromised. The low-loss composite structure of CMCD p

25、hase plugs increases sensitivity by more than 2 dB, as compared to a phase plug fabricated in expanded polystyrene. An Optimal Exit Diameter: Each CMCD features a 4-inch exit diameter to couple to a Progressive Transition (PT) midrange waveguide. The 4 inch exit provides two key advantages: First, c

26、ompared to a 2-inch or 3-inch exit, the 4- inch exit produces significantly lower air pressure at the throat. This lowers harmonic and intermodu- lation distortion dramatically. The distortion perfor- mance of each CMCD equals systems where the transducer couples directly to the waveguide throat. Se

27、condly, the 4-inch exit allows for waveguide coverage angles of up to 130 with a crossover points as high as 2-3kHz. Solutions with larger throat diameters have difficulty achieving 90 coverage with a 1 kHz crossover-point, in compari- son. Smaller Cone Diameter Transducers for Extended Bandwidth an

28、d High Sensitivity: Why did JBL choose to use smaller 8-inch and 6.5- inch transducers? The answer is that in a compres- sion & waveguide loaded midrange system, the diameter of the cone does not matter! With proper loading provided by an annular-ring phase plug, cone excursion is always extremely l

29、ow. The two parameters that determine sensitivity and band- width are moving mass and magnetic circuit strength. To provide wide bandwidth and high sensitivity, moving mass must be minimized, and motor strength must be maximized. Larger diameter drivers may provide high motor strength, but a larger

30、cone diameter fundamentally limits how low the moving mass can be. The midrange transducers at present are the 8- inch diameter 2250 and the 6.5-inch diameter 165H. The 2250 feature JBLs patented Neody- mium Differential Drive (NDD) technology, providing 350 watt power handling and half the power co

31、mpression of traditional designs. The 165H is an established high motor strength ce- ramic magnet design, featuring 125 watt power handling and an extremely low moving mass for extended high frequency bandwidth. As noted, the two parameters that dominate in determining sensitivity and usable bandwid

32、th are “motor strength”, or (BL)2/Re, and “moving mass”, Mms. Examining the industry standard 12-inch diameter JBL 2012, the 2250 has a higher (BL)2/ Re of 58.2 ohm compared to 41.5 ohm for the 2012. The moving masses of the two transducers are equal at 25 grams. Considering the higher motor strengt

33、h, and equal moving mass, we see 5 the 2250 is actually a higher sensitivity transducer, when the waveguide provides a sufficient acoustic impedance load. A similar analysis shows the 165H provides the same advantages over other industry comparable transducers. For comparison Figure 5 shows cut-away

34、 views of the 2012 and the 2250. Optimal Sized Thermal Conductive Rear Enclosures: Existing cone midrange horn-loaded systems often incorporate a large rear chamber typically filled with lossy damping material such as fiberglass or polyester wool. However, when a midrange device is loaded by a prope

35、rly designed annular ring phase plug and an appropriate midrange waveguide such a solution is not sufficient. To extend bandwidth to a lower frequency, the rear chamber must be sized for proper reactance nulling The acoustical air load (acoustic mass) provided by the waveguide and phasing plug must

36、be JBL 2012: JBL 2250: Figure 5: JBL 2012H, Traditional 12-inch High- Output Midrange driver. cancelled by the acoustic stiffness (acoustic compliance) of the rear enclosure of the midrange. Plach (Design Factors in Horn Type Speakers, JAES, October, 1953) shows that the rear enclo- sure then needs

37、to be very small. Any lossy absorp- tion in the rear enclosure reduces output in the lower frequency range. An optimally sized rear enclosure can be acoustically shaped to eliminate resonances within the enclosure, without using lossy damping materials. The result is ideal lower frequency bandwidth

38、and resonance-free response. The rear chambers are thermally conductive aluminum enclosures to allow heat from the motor structure to dissipate. This reduces power com- pression and increases power handling. This JBL proprietary technology was first employed in JBLs Venue Series. Other proven applic

39、ations include JBL LSR Studio Monitors, VerTec VT4889, and PD Precision Directivity Systems. CMCD rear chambers seal against the rear of the transducer frame, allowing heat to escape freely. In the CMCD-81, the entire NDD motor structure with its cooling fins is outside of the rear enclo- sure. In t

40、he CMCD-61, the entire backplate of the ceramic magnet structure is exposed to the surrounding air for better thermal performance. CMCD Advanced Technical Features: Correct spacing from the cone provides correct acoustic coupling. The result is optimal low volume velocity and high pressure at the co

41、ne. Uniform cone loading provided by CMCD phasing plugs ensures pistonic response, and extended bandwidth. A flat wavefront at the waveguide throat results from path length compensation. This ensures smooth and predictable on and off-axis re- sponse, and increased signal coherency. Optimal low frequ

42、ency loading results in increased LF bandwidth. Optimal cone/phase-plug spacing provides maximum mid-band sensitivity. Optimal slot gap-width, and slot location extends HF bandwidth by moving transverse 6 resonances between the cone and phase plug to a much higher frequency. A Moderate 7:1 compressi

43、on ratio provides low distortion performance, equaling that of designs such as JBL ScreenArray and PD systems that do not use phasing plugs. A 3 to 5 dB increase in sensitivity results, compared to systems that couple the trans- ducer directly to the waveguide throat, without a phasing plug. A 4-inc

44、h exit diameter provides low distortion performance, and allows extremely wide coverage angle horns to be designed. Technical and Subjective Performance: This section documents the performance of each CMCD, and compares the performance to existing solutions. The technical performance presented provi

45、des an examination of objective and subjec- tive performance features of CMCD designs. Plane-Wave Tube Response: Figure 6 shows acoustical power-response of a CMCD-81H, mounted to a 4-inch diameter plane- wave tube, 16 feet in length, as shown in Figure 7. Measuring the acoustic response of a compre

46、ssion driver on a plane-wave tube is equivalent to measuring the near-field response of a direct radiating transducer. The plane-wave tube isolates the response of the compression driver from the effects of a waveguide. Response anomalies seen on the plane-wave tube will likely show in the on- and o

47、ff-axis curves of the compression driver on a waveguide, and will likely be audible. Referring to Figure 6, note the high 30% efficiency of the CMCD-81H in converting electrical power to acoustical power. As well, note the smooth fre- quency response through the entire usable range from 200 Hz to 20

48、00 Hz. Coupled to a correct waveguide, we expect uniform frequency re- sponse, high sensitivity, and an uncolored sound quality. Figure 8 shows the plane-wave tube response of the CMCD-61H. 34% efficiency is achieved, and the acoustical response is free of resonances. Usable bandwidth extends from 3

49、50 Hz to 3.5 kHz. Figure 7: Photograph of 4.9 meter (16 foot) 4-inch diameter Plane-Wave Tube with CMCD-81. 7 100100010000 100 110 120 130 140 0.01 0.1 1 10 2020K SPL (dB) Frequency (Hz) Efficiency (%) 70 Figure 6: CMCD-81H Frequency Response, Measured on 4-inch Plain-Wave Tube at 1 Watt (2.83 Volts). 100100010000 100 110 120 130 140 0.01 0.1 1 10 20 20K SPL (dB) Frequency (Hz) Efficiency (%) 70 Figure 8: CMCD-61H Frequency Response, Measured on 4-inch Plain-Wave Tube at 1 Watt (2.83 Volts). Plane-Wave Tube - SPL and Efficiency Plane-Wave Tube - SPL and Efficiency 8 Non-Linear Dis