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LM4950TS Datasheet(PDF) 17 Page - National Semiconductor (TI) |
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LM4950TS Datasheet(HTML) 17 Page - National Semiconductor (TI) |
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17 / 25 page ![]() Application Information (Continued) SELECTING EXTERNAL COMPONENTS Input Capacitor Value Selection Two quantities determine the value of the input coupling capacitor: the lowest audio frequency that requires amplifi- cation and desired output transient suppression. As shown in Figure 3, the input resistor (R IN) and the input capacitor (C IN) produce a high pass filter cutoff frequency that is found using Equation (7). f c = 1/2 πR iCi (7) As an example when using a speaker with a low frequency limit of 50Hz, C i, using Equation (7) is 0.159µF. The 0.39µF C INA shown in Figure 3 allows the LM4950 to drive high efficiency, full range speaker whose response extends below 30Hz. Bypass Capacitor Value Besides minimizing the input capacitor size, careful consid- eration should be paid to value of C BYPASS, the capacitor connected to the BYPASS pin. Since C BYPASS determines how fast the LM4950 settles to quiescent operation, its value is critical when minimizing turn-on pops. The slower the LM4950’s outputs ramp to their quiescent DC voltage (nomi- nally V DD/2), the smaller the turn-on pop. Choosing CBYPASS equal to 10µF along with a small value of C IN (in the range of 0.1µF to 0.39µF), produces a click-less and pop-less shut- down function. As discussed above, choosing C IN no larger than necessary for the desired bandwidth helps minimize clicks and pops. OPTIMIZING CLICK AND POP REDUCTION PERFORMANCE The LM4950 contains circuitry that eliminates turn-on and shutdown transients ("clicks and pops"). For this discussion, turn-on refers to either applying the power supply voltage or when the micro-power shutdown mode is deactivated. As the V DD/2 voltage present at the BYPASS pin ramps to its final value, the LM4950’s internal amplifiers are configured as unity gain buffers and are disconnected from the AMP A and AMP B pins. An internal current source charges the ca- pacitor connected between the BYPASS pin and GND in a controlled manner. Ideally, the input and outputs track the voltage applied to the BYPASS pin. The gain of the internal amplifiers remains unity until the voltage applied to the BY- PASS pin. The gain of the internal amplifiers remains unity until the voltage on the bypass pin reaches V DD/2. As soon as the voltage on the bypass pin is stable, the device becomes fully operational and the amplifier outputs are reconnected to their respective output pins. Although the BYPASS pin cur- rent cannot be modified, changing the size of C BYPASS alters the device’s turn-on time. Here are some typical turn-on times for various values of C BYPASS: C B (µF) T ON (ms) 1.0 120 2.2 120 4.7 200 10 440 In order eliminate "clicks and pops", all capacitors must be discharged before turn-on. Rapidly switching V DD may not allow the capacitors to fully discharge, which may cause "clicks and pops". There is a relationship between the value of C IN and C BYPASS that ensures minimum output transient when power is applied or the shutdown mode is deactivated. Best perfor- mance is achieved by setting the time constant created by C IN and Ri +Rf to a value less than the turn-on time for a given value of C BYPASS as shown in the table above. DRIVING PIEZO-ELECTRIC SPEAKER TRANSDUCERS The LM4950 is able to drive capacitive piezo-electric trans- ducer loads that are less than equal to 200nF. Stable opera- tion is assured by placing 33pF capacitors in parallel with the 20k Ω feedback resistors. The additional capacitors are shown in Figure 4. When driving piezo-electric tranducers, sound quality and accoustic power is entirely dependent upon a transducer’s frequency response and efficiency. In this application, power dissipated by the LM4950 is very low, typically less than 250mW when driving a 200nF piezo-electric transduce (V DD = 12V). www.national.com 17 |
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