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LM4881M датащи(PDF) 8 Page - National Semiconductor (TI) |
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LM4881M датащи(HTML) 8 Page - National Semiconductor (TI) |
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8 / 11 page ![]() Application Information SHUTDOWN FUNCTION In order to reduce power consumption while not in use, the LM4881 contains a shutdown pin to externally turn off the amplifier’s bias circuitry. This shutdown feature turns the am- plifier off when a logic high is placed on the shutdown pin. The trigger point between a logic low and logic high level is typically half supply. It is best to switch between ground and supply to provide maximum device performance. By switch- ing the shutdown pin to the V DD, the LM4881 supply current draw will be minimized in idle mode. While the device will be disabled with shutdown pin voltages less than V DD, the idle current may be greater than the typical value of 0.7 µA. In ei- ther case, the shutdown pin should be tied to a definite volt- age because leaving the pin floating may result in an un- wanted shutdown condition. In many applications, a microcontroller or microprocessor output is used to control the shutdown circuitry which provides a quick, smooth tran- sition into shutdown. Another solution is to use a single-pole, single-throw switch in conjunction with an external pull-up re- sistor. When the switch is closed, the shutdown pin is con- nected to ground and enables the amplifier. If the switch is open, then the external pull-up resistor will disable the LM4881. This scheme guarantees that the shutdown pin will not float which will prevent unwanted state changes. POWER DISSIPATION Power dissipation is a major concern when using any power amplifier and must be thoroughly understood to ensure a successful design. Equation 1 states the maximum power dissipation point for a single-ended amplifier operating at a given supply voltage and driving a specified output load. P DMAX =(VDD) 2 /(2 π2R L) (1) Since the LM4881 has two operational amplifiers in one package, the maximum internal power dissipation point is twice that of the number which results from Equation 1. Even with the large internal power dissipation, the LM4881 does not require heat sinking over a large range of ambient tem- perature. From Equation 1, assuming a 5V power supply and an 8 Ω load, the maximum power dissipation point is 158 mW per amplifier. Thus the maximum package dissipation point is 317 mW. The maximum power dissipation point obtained must not be greater than the power dissipation that results from Equation 2: P DMAX =(TJMAX −TA)/ θJA (2) For package MUA08A, θ JA = 230˚C/W, and for package M08A, θ JA = 170˚C/W, and for package N08E, θ JA = 107˚C/W. T JMAX = 150˚C for the LM4881. Depending on the ambient temperature, T A, of the system surroundings, Equa- tion 2 can be used to find the maximum internal power dissi- pation supported by the IC packaging. If the result of Equa- tion 1 is greater than that of Equation 2, then either the supply voltage must be decreased, the load impedance in- creased or T A reduced. For the typical application of a 5V power supply, with an 8 Ω load, the maximum ambient tem- perature possible without violating the maximum junction temperature is approximately 96˚C provided that device op- eration is around the maximum power dissipation point. Power dissipation is a function of output power and thus, if typical operation is not around the maximum power dissipa- tion point, the ambient temperature may be increased ac- cordingly. Refer to the Typical Performance Characteris- tics curves for power dissipation information for lower output powers. POWER SUPPLY BYPASSING As with any power amplifer, proper supply bypassing is criti- cal for low noise performance and high power supply rejec- tion. The capacitor location on both the bypass and power supply pins should be as close to the device as possible. As displayed in the Typical Performance Characteristics sec- tion, the effect of a larger half supply bypass capacitor is im- proved low frequency PSRR due to increased half-supply stability. Typical applications employ a 5V regulator with 10 µF and a 0.1 µF bypass capacitors which aid in supply stability, but do not eliminate the need for bypassing the sup- ply nodes of the LM4881. The selection of bypass capaci- tors, especially C B, is thus dependent upon desired low fre- quency PSRR, click and pop performance as explained in the section, Proper Selection of External Components section, system cost, and size constraints. PROPER SELECTION OF EXTERNAL COMPONENTS Selection of external components when using integrated power amplifiers is critical to optimize device and system performance. While the LM4881 is tolerant of external com- ponent combinations, consideration to component values must be used to maximize overall system quality. The LM4881 is unity gain stable and this gives a designer maximum system flexibility. The LM4881 should be used in low gain configurations to minimize THD+N values, and maximum 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 dicated by the choice of external components shown in Figure 1. Both the input coupling capacitor, C i, and the out- put coupling capacitor, C o, form first order high pass filters which limit low frequency response. These values should be chosen based on needed frequency response for a few dis- tinct reasons. Selection of Input and Output Capacitor Size Large input and output capacitors are both expensive and space hungry for portable designs. Clearly a certain sized capacitor is needed to couple in low frequencies without se- vere attenuation. But in many cases the speakers used in portable systems, whether internal or external, have little ability to reproduce signals below 150 Hz. Thus using large input and output capacitors may not increase 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 and output capacitor sizes, careful consideration 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 LM4881 turns on. The slower the LM4881’s outputs ramp to their quiescent DC voltage (nominally 1/2 V DD), the smaller the turn on pop. Thus choosing C B equal to 1.0 µF along with a small value of C i (in the range of 0.1 µF to 0.39 µF), the www.national.com 8 |
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