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MP1740 Datasheet(PDF) 9 Page - Monolithic Power Systems |
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MP1740 Datasheet(HTML) 9 Page - Monolithic Power Systems |
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9 / 11 page ![]() MP1740 –3W HIGH EFFCIENCY MONO CLASS-D AUDIO AMPLIFIER MP1740 Rev. 1.0 www.MonolithicPower.com 9 1/5/2012 MPS Proprietary Information. Unauthorized Photocopy and Duplication Prohibited. © 2012 MPS. All Rights Reserved APPLICATION INFORMATION COMPONENT SELECTION The MP1740 uses a minimum number of external components to complete a fully bridged Class D audio amplifier. Use the following sections to customize the amplifier for your particular application. 1. Setting the Voltage Gain The voltage gain sets the output voltage swing for a given input voltage swing and is set by the input resistors (RI) as the following equation: I 150kΩ GAIN=2 R × (1) The maximum output voltage swing is limited by the power supply. To achieve the maximum output power of the MP1740 amplifier, set the amplifier gain such that the maximum peak-to- peak input signal results in at least the maximum peak-to-peak output voltage swing. Lower gain allows the MP1740 to operate at its best, because a higher voltage at the input for the same output power making the inputs less susceptible to noise. So setting voltage gain to 2V/V may achieve optimal performance. 2. Input Coupling Capacitors (CI) The MP1740 is a mono BTL Class-D amplifier with differential inputs and outputs. This device can still be used with a single-ended input; but for some noisy environment (such as a wireless handset) the MP1740 should be used with differential inputs to ensure maximum noise rejection. The fully differential amplifier allows the inputs to be biased at voltage other than mid-supply. The input coupling capacitors are not required if the design uses a differential source that is biased from 0.5 V to VCC - 0.8 V (as shown in Recommended Operating Conditions). If the input signal is not biased within the recommended common-mode input range or if using a single-ended source, the input coupling capacitors are used to pass only the AC audio signal to the input of the amplifier as a high pass filter. The input capacitors create a high-pass filter with the input resistor. Choose an input coupling capacitor such that the corner frequency fC is less than the desired pass-band frequency. The formula for the corner frequency is: C II 1 f= 2πRC (2) Speakers in wireless handsets usually can’t respond well to low frequencies, so for this application the corner frequency can be set to block the low frequencies. The input coupling capacitance is calculated as: I IC 1 C= 2πRf (3) If the corner frequency is within the audible band, the capacitors should have a tolerance of ±10% or better, because any mismatch in capacitance causes an impedance mismatch at the corner frequency and below. 3. Power Supply Decoupling Capacitor (CS) The class-D audio amplifier requires adequate power supply decoupling to ensure the efficiency is high and total harmonic distortion (THD) is low. To carry the higher frequency transient current, spikes, or digital hash on the line, a good low ESR ceramic capacitor is necessary. Place a 1μF decoupling capacitor as close as possible to the device VCC lead. It is very important for the efficiency of the class-D amplifier, because any resistance or inductance in the trace between the capacitor and the device may cause a loss. A 10μF or greater capacitor placed near the audio power amplifier would also help for filtering lower- frequency noise. 4. Input Resistors (RI) In fully differential amplifiers, please use the matching input resistors. Matching is very important for the balance of the output on the reference voltage (more important than overall tolerance). The higher matching, the batter CMRR and PSRR performance. Therefore, it is recommended to use 1% precision resistors or better to keep the performance optimized. Place the input resistors as close to the MP1740 as possible to limit noise injection on the high- impedance nodes. |
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