Qsc - Pl90Wp 电路图.pdf
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1、1 The PowerLight 9.0PFC High-Power Innovations in Audio Amplifier Technology Sometimes the magnitude of a task requires tossing aside conventional technologies used for smaller, easier undertakings, and instead developing and adapting new ones to suit. QSCs engineers faced such a situation developin
2、g the Power-Light 9.0PFC, the first high-power professional audio amplifier to feature power factor correction, a very prominent feature among other “firsts” and “mosts.” Responding to the growing demand in the sound reinforce- ment industry for more powerful and reliable amplification in smaller an
3、d lighter packaging, our PowerLight 9.0PFC design team took on no small challenge: to develop an amplifier that delivers at least twice the power of one of the worlds most powerful amplifiersthe PowerLight 4.0without sacrificing the rack size and ratio of watts per pound. And of course, the team cou
4、ldnt compromise audio performance in any way. The design teams job was to develop a new class of amplifier whose power is measured in thousands of watts, rather than hundreds. The result is the most innovative and advanced amplifier on the planet, delivering up to 9000 watts of undistorted power. Th
5、e objective of this paper is to take the reader behind the curtains and explain the basic technology and its benefits to the pro audio user. The amplifier: new devices, new techniques Seeking to double the 4.0s power output in the same size package, we quickly saw that we could not simply scale up t
6、he familiar bipolar transistor designs that have served us well at lower powers. It would simply take too many devices and too much heat sink area to do the job. No, this required a new class of device. The most rapidly advancing class of power devices today is the N-channel power metal oxide semico
7、nductor field-effect transistor (MOSFET), currently used primarily for high-power switching supplies; this application requires devices with very high speed, capable of handling high currents and high volt- ages, and having low on-resistance. Coincidentally, these properties also make them suitable
8、for high-performance audio amplification. The power MOSFET supplies an unmatched combination of very high peak voltage and current capability, together with uniform gain. Among the broad choice of device ratings are large-die transistors that individually can replace several bipolar devices. Further
9、more, the power MOSFET has no “second breakdown” region, which has historically limited the maximum power potential of bipolar devices. The power handling capacity of the MOSFET is limited strictly by the thermal capacity of the device package and the heat sink structure it is attached to, which can
10、 be made as heavy as required. For the PowerLight 9.0PFC, we determined that eight latest-generation, large-die MOSFETs can replace a bank of 56 bipolar devices, with equal or better energy handling ability. Dont confuse the N-channel MOSFET with the lateral type that has been used for years in many
11、 traditional linear audio amplifiers. The lateral devices, although available in both polarities, have inherently lower current and efficiency limits. Although simple moderate-power-level designs utilizing lateral MOSFETs have been successful, their per-device power capacity is no better than tradit
12、ional bipolar devices, and 500110100 1 10 100 Collector current (I ) Drain current (I ) in amperes C D Collector-emitter voltage (V ) Drain-source voltage (V ) CE DS PowersMOSFETafe operating area (SOA) Power bipolar device safe operating area (SOA) SOA comparison of power devices RadioFans.CN 收音机爱
13、好者资料库 2 their efficiency is somewhat lower. The switching-type, N- channel MOSFET employed in the PowerLight 9.0PFC, on the other hand, has far lower on-losses and far greater current capacity. There are two main obstacles to using N-channel MOSFETs effectively: their turn-on thresholds vary widely
14、from one device to another; and they can only be produced effectively in N-channel polarity. The threshold variations would tend to result in uncontrollable idle current and possible crossover distortion, and the single polarity requires a new circuit concept to produce a fully complementary, matche
15、d positive and negative output signal. To solve the problems we developed a fundamentally superior amplifier architecture that we call Full-Bridge Current Cell topology. The current cell concept Current cell topology solves both problems by enclosing each FET within closed-loop active circuitry to c
16、reate a predictable relationship between input signal and output current. This support circuitry converts the real-world device, despite its variables, into an ideal circuit element with zero turn-on threshold and better than 1% linearity. In effect, it creates the ideal device that every audio engi
17、neer has dreamed of. Cell elements are matched to within 1%, making low- distortion arrays easy to configure. Deploying these cells in a conventional half bridge would require dual matching positive and negative power supplies in order to produce a symmetrical output signal. Because of the high powe
18、r requirements, though, the PowerLight 9.0PFC uses four dual current cells on each channel in an internally grounded, full-bridge configuration, which also simplifies the power supply structure, as well discuss later. The full-bridge topology has a balanced, fully symmetrical power flow, and it deli
19、vers positive and negative output voltages from a common power supply reservoir. Furthermore, it balances out certain residual distortion mechanisms from the audio signal. When combined with the four-step Class H rail control scheme described below, the result is a very high power linear output stag
20、e with an efficiency approaching that of a Class D (pulse- width modulation) amplifier. Class B signal conversion Getting good results even with ideal current cells required another innovation: a perfect Class A-to-B converter. Audio from the input stage is in the form of a Class A signal, a continu
21、ous voltage which varies symmetrically between positive and negative limits. For optimum efficiency, we need to split this single continuous signal into perfectly matched positive and negative halves, so the resulting Class B signals can be routed to their respective current cells. In a conventional
22、 amplifier, this polarity split is done with moderate accuracy using complementary positive- and negative- polarity transistors, carefully biased so they “just meet” at zero. The positive transistor handles the positive half of the wave- form and ignores the negative half, and the negative transisto
23、r does the opposite. In most cases, it works acceptably well, although the center matching is somewhat imprecise and thermally variable, requiring carefully designed thermal compensation circuits to maintain a good trade-off between acceptably low crossover distortion (zero-crossing errors) and exce
24、ssive idle current. Also, because the bipolar scheme uses two separate amplifying transistors, the cumulative component tolerances can cause a mismatch between the positive and negative halves. There are also breakdown situations in which both devices might amplify at the same time, leading to a cat
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