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LM4871M 数据表(PDF) 6 Page - National Semiconductor (TI) |
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LM4871M 数据表(HTML) 6 Page - National Semiconductor (TI) |
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6 / 8 page ![]() Application Information (Continued) external component combinations, consideration to compo- nent values must be used to maximize overall system qual- ity. The LM4871 is unity-gain stable which gives a designer maximum system flexibility. The LM4871 should be used in low gain configurations to minimize THD+N values, and maximize the signal to noise ratio. Low gain configurations require large input signals to obtain a given output power. In- put signals equal to or greater than 1 Vrms are available from sources such as audio codecs. Please refer to the sec- tion, Audio Power Amplifier Design, for a more complete explanation of proper gain selection. Besides gain, one of the major considerations is the closed- loop bandwidth of the amplifier. To a large extent, the band- width is dictated by the choice of external components shown in Figure 1. The input coupling capacitor, C i, forms a first order high pass filter which limits low frequency re- sponse. This value should be chosen based on needed fre- quency response for a few distinct reasons. Selection Of Input Capacitor Size Large input capacitors are both expensive and space hungry for portable designs. Clearly, a certain sized capacitor is needed to couple in low frequencies without severe attenua- tion. But in many cases the speakers used in portable sys- tems, whether internal or external, have little ability to repro- duce signals below 100 Hz to 150 Hz. Thus, using a large input capacitor may not increase actual system perfor- mance. In addition to system cost and size, click and pop perfor- mance is effected by the size of the input coupling capacitor, C i. A larger input coupling capacitor requires more charge to reach its quiescent DC voltage (nominally 1/2 V DD). This charge comes from the output via the feedback and is apt to create pops upon device enable. Thus, by minimizing the ca- pacitor size based on necessary low frequency response, turn-on pops can be minimized. Besides minimizing the input capacitor size, careful consid- eration should be paid to the bypass capacitor value. Bypass capacitor, C B, is the most critical component to minimize turn-on pops since it determines how fast the LM4871 turns on. The slower the LM4871’s outputs ramp to their quiescent DC voltage (nominally 1/2 V DD), the smaller the turn-on pop. Choosing C B equal to 1.0 µF along with a small value of Ci (in the range of 0.1 µF to 0.39 µF), should produce a virtually clickless and popless shutdown function. While the device will function properly, (no oscillations or motorboating), with C B equal to 0.1 µF, the device will be much more susceptible to turn-on clicks and pops. Thus, a value of C B equal to 1.0 µF is recommended in all but the most cost sensitive de- signs. AUDIO POWER AMPLIFIER DESIGN Design a 1W/8 Ω Audio Amplifier Given: Power Output 1 Wrms Load Impedance 8 Ω Input Level 1 Vrms Input Impedance 20 k Ω Bandwidth 100 Hz–20 kHz ± 0.25 dB A designer must first determine the minimum supply rail to obtain the specified output power. By extrapolating from the Output Power vs Supply Voltage graphs in the Typical Per- formance Characteristics section, the supply rail can be easily found. A second way to determine the minimum sup- ply rail is to calculate the required V opeak using Equation 3 and add the output voltage. Using this method, the minimum supply voltage would be (V opeak +(VODTOP +VODBOT)), where V ODBOT and VODTOP are extrapolated from the Dropout Volt- age vs Supply Voltage curve in the Typical Performance Characteristics section. (3) Using the Output Power vs Supply Voltage graph for an 8 Ω load, the minimum supply rail is 4.6V. But since 5V is a stan- dard voltage in most applications, it is chosen for the supply rail. Extra supply voltage creates headroom that allows the LM4871 to reproduce peaks in excess of 1W without produc- ing audible distortion. At this time, the designer must make sure that the power supply choice along with the output im- pedance does not violate the conditions explained in the Power Dissipation section. Once the power dissipation equations have been addressed, the required differential gain can be determined from Equa- tion 4. (4) R f/Ri = AVD/2 (5) From Equation 4, the minimum A VD is 2.83; use AVD =3. Since the desired input impedance was 20 k Ω, and with a A VD impedance of 2, a ratio of 1.5:1 of Rf to Ri results in an allocation of R i =20kΩ and Rf =30kΩ. The final design step is to address the bandwidth requirements which must be stated as a pair of −3 dB frequency points. Five times away from a −3 dB point is 0.17 dB down from passband response which is better than the required ±0.25 dB specified. f L = 100 Hz/5 = 20 Hz f H =20kHz*5=100 kHz As stated in the External Components section, R i in con- junction with C i create a highpass filter. C i ≥ 1/(2π*20 kΩ*20 Hz) = 0.397 µF; use 0.39 µF The high frequency pole is determined by the product of the desired frequency pole, f H, and the differential gain, AVD. With a A VD = 3 and fH = 100 kHz, the resulting GBWP = 150 kHz which is much smaller than the LM4871 GBWP of 4 MHz. This figure displays that if a designer has a need to design an amplifier with a higher differential gain, the LM4871 can still be used without running into bandwidth limi- tations. www.national.com 6 |
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