JBL Technical Note - Vol.1, No.24 电路原理图.pdf

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1、Introduction: The desired performance features for dedicated midrange cone transducers are: 1. Extended power response; rising axial response 2. High electromechanical coupling (high efficiency) 3. Bandpass optimization (low mass; high resonance) 4. Low distortion at target operating levels 5. Adapt

2、ability to both direct radiator and horn use 6. High reliability In this Tech Note we will discuss two new products, models 2012H 200 mm (10 in) and 2020H 250 mm (12 in), that meet these performance requirements in their respective size categories. These devices also have suspension elements and exc

3、ursion (XMAX) capabilities that allow use in certain LF applications as well. These transducers have been designed for maximum output, with a combination of extended power response with rising on-axis response, and a combination of efficiency, sensitivity, power handling, and low dynamic power compr

4、ession that make them ideal as mid and low- midrange horn drivers, as well as for low frequency use as direct radiators in stage monitors. These transducers join the 2227H 300 mm (15 in) and 2242H 380 mm (18 in) SVG (Super Vented Gap) transducers in the Maximum Output Series (see Technical Notes Vol

5、ume 1, Number 22). Overview of Design: Both models use a new magnetic structure with a heavy copper sleeve symmetrically positioned on the polepiece above and below the top plate. The copper sleeve is in the voice coil gap and functions as a shorting ring, substantially reducing second and third har

6、monic components arising from nonlinearities in the magnetic circuit as it is modulated by the voice coil signal current. In JBLs traditional SFG (Symmetrical Field Geometry) motor structures, an aluminum shorting ring at the base of the polepiece reduces second harmonic distortion; saturated, under

7、cut pole tips are then used to reduce third harmonic distortion. Saturation reduces magnetic energy in the gap resulting in a loss of flux density. In the new design a larger gap is required to accommodate the copper ring, and the flux loss resulting from this is about the same as with the use of sa

8、turated pole tips. The advantage here is that both second and third harmonic are now reduced by a single design element. The copper ring has another advantage; acting as a shorted secondary turn on a transformer (the voice coil is the primary winding), the normal rise in voice coil impedance at high

9、er frequencies is vastly reduced as the low resistance of the shorted turn is reflected through to the primary side. This means that substantially less voltage is required to maintain flat response at the upper end of the transducers passband. Further refinements in the moving system complete the de

10、sign. Attention is given to cone and suspension materials to reduce breakup and increase overall mechanical linearity. Attention has also been given to matters of heat transfer, and dynamic power compression has been minimized. Mechanical Details of the Design: Figure 1 shows a section view of the 2

11、020H magnet structure. The copper sleeve placed over the polepiece can clearly be seen, with the voice coil located just outside the sleeve. Note that the polepiece extends slightly beyond the upper surface of the top plate. The materials comprising the cone, surround, and inner compliance (spider)

12、have all been chosen and formed for high excursion with minimum mechanical breakup over the normal passband of the transducer. Technical Notes, Volume 1, Number 24 JBLs New Maximum Output, Midrange/Low-Frequency Transducers 1 Figure 1. Section view of 2020H magnet structure. Top Plate Magnet Figure

13、3. 2020H at one-tenth rated power (30 W); 2nd (dashed) and 3rd (dotted) harmonics raised 20 dB. Pole Piece Impedance Control: Performance of the Transducers: Distortion: The extremely low midband distortion of the 2012H is shown in Figure 2. Here, the transducer was placed in JBLs standard 290 liter

14、 (10 cu ft) sealed enclosure, in which any transducer with high electromechanical coupling will show a highly damped (rolled off) low frequency response. Input power was set at 0.1 rated power, 30 watts, attaining a midband level at one meter of 114 dB SPL. Note the extremely smooth, gradually risin

15、g response over the transducers target operating range from 100 Hz to 2500 Hz. Over this frequency interval the values of second and third harmonic distortion do not rise above a value of 2%. Even more to the point, the distortion in the lower midrange from 100 to 600 Hz is below 1 %. Figure 3 shows

16、 data for the 2020H under similar conditions at 0.1 rated power (30 watts), attaining a level of 117 dB. Note the very low distortion over the frequency range from 80 Hz to 4 kHz. Over this frequency interval the distortion remains below 3%; over the range from 100 to 600 Hz the distortion remains b

17、elow 1%. In both designs, the level of 3rd harmonic distortion remains extremely low, normally well below 1 % except at very low frequencies where the nonlinearity of the cone compliance elements becomes evident. Figure 2. 2012H at one-tenth rated power (30 W); 2nd (dashed) and 3rd (dotted) harmonic

18、s raised 20 dB. The impedance magnitude for the 2012H transducer is shown in Figure 4. The impedance is stabilized at 8 ohms over the range from about 200 Hz to 4 kHz. The dashed curve in Figure 4 shows the typical rise in impedance at mid and high frequencies in the absence of a shorting ring adjac

19、ent to the voice coil. In the frequency range above 250 Hz, the transducer presents a uniform resistive load. This results in maximum efficiency of coupling the amplifier to the load, and presents as well an easy load for the amplifier to drive. Figure 4. Impedance modulus for 2012H (solid curve); d

20、ashed curve shows typical rise in impedance modulus for a transducer without a copper sleeve. Dynamic Compression: Very few manufacturers of professional transducers routinely present performance data on power compression. Power compression results from the increase in voice coil temperature and the

21、 consequent rise in its dc resistance. When this occurs there is less power drawn from the amplifier during peak signal periods. In making power compression measurements, a 60 - 600 Hz band of pink noise with a crest factor of 6 dB is applied to the transducer at the designated power level. The tran

22、sducer is then preconditioned for a period of 5 minutes at that level, and an output SPL reading is taken. This is compared with the theoretical output SPL at that power level assuming that there is no power compression present. Power compression at high operating levels has the effect of robbing mu

23、sic of its essential dynamics, sounding somewhat as though a limiter/compressor has been added to the system. Power compression is normally accompanied by a shift in LF alignment that tends to make the response somewhat boomy and less controlled. 2 Back Plate Copper Sleeve fundamental, 14.55V 2nd +2

24、MB 3M20dB SPL,(dB) Frequency (Hz) 2012H Impedance Reaponae Conventional Dnw Impedance Reeponse Impedance (Ohms) Frequency (Hz) fundamental. 14.55V 2nd+20dB 3rd+20dB Frequency (Hz) SPL.(dB) JBL presents this data as a guide to professional users who are concerned with performance under long-term peri

25、ods of continuous usage at or near rated power: Figure 6. Example of horn loading of the 2012H in the Venue Series systems. Views of a typical mid-bass horn (a); on-axis response of the horn shown at (b) with the 2012H driver through the MF bandpass section of the dividing network. (1 W input measur

26、ed at 1 m). Applications: Horn loading: The 2012H and 2020H transducers are intended for both direct radiating and horn loaded applications. For horn loading, Keeles data shown in Figure 5, will be useful. Here, the region of flat power response on a proper horn design will be bounded by fL C at low

27、 frequencies and fH M at high frequencies. The various breakpoints in the graph are given as: f LC = (CUV2 fM = 2(fs)/Qts fH C = (2Qts)fs(Vas/Vfc) Where: Qt s = total Q of the transducer fs = free-air resonance of the transducer Re = voice coil dc resistance (in ohms) Lg = voice coil inductance (in

28、henrys) Va s = volume of air that provides a restoring force equal to that of the transducers mechanical compliance (in liters) Vf c = volume of the horns front air chamber (in liters) All of the quantities needed in determining the various breakpoints can be taken from the listing of the Thiele-Sma

29、ll parameters for the two transducers. Vfc is dependent on the horn design. Typical horn usage of the 2012H transducer in the JBL Venue Series Model 3215-9 MF section is shown in Figure 6. Note the smooth response over the interval from 300 Hz to 1 kHz and the output sensitivity of 106 dB, 1 W at 1

30、m. Figure 5. Thiele-Small parameters for LF horn applications, as developed by Keele. Log frequency (Hz) (a) VS3215 Midrange Section (b) Direct Radiator Use; Typical Low Frequency Alignments: Because of their relatively high resonances and very low Qt s values, the 2012H and 2020H can be mounted in

31、fairly small enclosures while maintaining smooth, peak free response. These small volume alignments normally present slightly rolled off LF response that may be easily equalized as needed. Applications may include direct radiator array elements or stage monitors. Typical LF alignments for these appl

32、ication are shown in Figure 7. Specifications 2012H: 2020H: Nominal Diameter 250 mm (10) 300 mm (12) Rated Impedance 8 ohms 8 ohms Power Capacity 1: 300 watts 300 watts Sensitivity, 1 W, 1 m (3.3)2; 100 dB 103 dB Frequency range 3: 75 Hz to 7 kHz 50 Hz to 5.5 kHz Power Compression 4: -10 dB power (3

33、0 W) 0.6 dB 0.5 dB -3 dB power (150W) 2.0 dB 1.7 dB rated power (300 W) 3.4 dB 2.8 dB Distortion 5: 2nd harmonic: 1.0% 1.0% 3rd harmonic: 1.0% 1.0% Highest recommended xover: 5.5 kHz 5 kHz Recommended enclosure volume: 10-301 (.35 - 1.05 ft3) 30 - 90 I (1.05 - 3.2 ft3) Effective piston diameter: 199

34、 mm (7.8 in) 260 mm (10.2 in.) Model: Compression at: Rated power: -3 dB: -10 dB: 2012H 2020H 3.4 dB 2.8 dB 2.0 dB 1.7 dB 0.6 dB 0.5 dB Table 1 SPL, 1W/1m(dB) Frequency (Hz) Relative response (dB) 6dB/octave im-mmm 12dBfodave 3 Thiele-Small Parameters 6: IAES standard (60-600 for 2020H, 100-1000 for

35、 2012H) sSensitivity is based on a swept 500 - 2500 Hz signal for an input of 2.83 V 8 ohms Frequency range is defined as the frequency extremes over which the response is -10 dB relative to the rated sensitivity Power compression is the sensitivity loss at the specified power, measured from 50 to 5

36、00 Hz, after a 5 minute AES standard pink noise preconditioning period test at the specified power sDistortion is measured at -10 dB rated power, from 100 to 500 Hz eThiele-Small parameters are measured after a 2-hour exercise period using a 300 W AES power test and reflects the expected long-term p

37、arameters once the driver has been installed and operated for a short period of time. Figure 7. Typical examples of the 2012H and 2020H transducers used in small ported enclosures. 2012H in a 0.3 cf (8.5 liter) enclosure tuned to 75 Hz (a); 2020H in a 1.5 cf (42.4 liter) enclosure tuned to 40 Hz (b)

38、; 2020H in a 1.1 cf (31 liter) enclosure tuned to 50 Hz (c); and 2020H in a 0.8 cf (22.6 liter) enclosure tuned to 60 Hz (d). u 61 Hz 60 Hz Re: 4.7 ohms 4.8 ohms a* 0.21 .23 aw 4 4.6 0.22 .24 31 liters (1.1 W) 65 liters (2.3 fP) SD: .031 m2 (48 in*) .053 m2 (82 in*) X MAX: 5 mm (0.2 in) 5 mm (0.2 in

39、) VD: 155 cm* (9.4 in3) 265 cms (16.75 itf) L,: Purely resistive at 1 kHz % (half-space): 3.1% 5.32% 300 W 300 W continuous pink noise, continuous pink noise, 100 Hztol kHz 60 Hz to 600 kHz (b, c,d) Reference: Keele, D., Low Frequency Horn Design Using Thiele-Small Driver Parameters, AES Preprint 12

40、50 (presented at the 51st AES Convention, Los Angeles, May 1977). JBL Professional 8500 Balboa Boulevard, P.O. Box 2200 Northridge, California 91329 U.S.A. H A Harman International Company TN Vol 1 No 24 CRP5M 9/98 Maximum excursion before damage (peak-to-peak): 16 mm (0.65 in) 16 mm (0.65 in) Minim

41、um impedance: 7 ohms 7 ohms Voice Coil Diameter: 76 mm (3 in) 76 mm (3 in) Voice Coil Material: Edgewound Aluminum Ribbon Voice Coil Winding Depth: 20.3 mm (0.8 in) 15.2 mm (0.6 in) Magnetic Gap Depth: 12.6 mm (0.5 in) 12.7 mm (0.5 in) Magnetic Assembly Weight: 7.7 kg (17 lb) 7.7 kg (17 lb) Bl facto

42、r: 15.5 Tm 18.3Tm Effective Moving Mass: 30 g 44g Polarity: EIA (positive voltage to RED terminal gives forward displacement SPL. 1Vv71m (dB) Frequency (Hz) JBL2012 75Hz. 0.3 cl (a) SPL, 1W/1m (dB) JBL2020 40Hz, 1.5cf JBL2020 50Hz, 1.1cf JBL2020 60Hz,0.8cf Frequency (Hz) Overall diameter: 237 mm (9.

43、33 in) sq.311 mm (12.2 in) 261mm (10.25 in) round Bolt circle diameter: 245 mm (9.623 in) 294 mm (11.6 in) Baffle cutout diameter: front mount: 229 mm 280 mm (9.0 in) (11.0 in) rear mount: 222 mm 284 mm (8.75 in) (11.2 in) Depth: 117 mm (4.6 in) 152 mm (6 in) Volume displaced by driver: 2.15 liters (.076 cu ft) 4 liters (0.11 cu ft) Net weight: 8.6 kg (19 lb) 8.6 kg (19 lb) Shipping weight: 9.1 kg (20 lb) 9.5 kg (21 lb) Mounting Information: 4