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MP7740 Datasheet(PDF) 8 Page - Monolithic Power Systems |
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MP7740 Datasheet(HTML) 8 Page - Monolithic Power Systems |
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8 / 12 page ![]() MP7740 – 15W CLASS D MONO SINGLE ENDED AUDIO AMPLIFIER MP7740 Rev. 0.9 www.MonolithicPower.com 8 9/22/2009 MPS Proprietary Information. Unauthorized Photocopy and Duplication Prohibited. © 2009 MPS. All Rights Reserved. APPLICATION INFORMATION COMPONENT SELECTION The MP7740 uses a minimum number of external components to complete a stereo Class D audio amplifier. The circuit of Figure 1 should be suitable for most applications, and use the following sections to determine how to customize the amplifier for a particular application. Setting the Voltage Gain The maximum output voltage swing is limited by the power supply. To achieve the maximum power out of the MP7740 amplifier, set the gain such that the maximum input signal results in the maximum output voltage swing. The maximum output voltage swing is ±VDD/2. For a given input signal voltage, where VIN (pk) is the peak input voltage, the maximum voltage gain is: ) pk ( V 2 V ) MAX ( A IN DD V × = This voltage gain setting results in the peak output voltage approaching it’s maximum for the maximum input signal. In some cases the amplifier is allowed to overdrive slightly, allowing the THD to increase at high power levels, and so a higher gain than AV (max) is required. Setting the Switching Frequency The idle switching frequency (the switching frequency when no audio input is present) is a function of several variables: the supply voltage VDD, the timing capacitor CINT and the feedback resistor RFB. Lower switching frequencies result in more inductor ripple, causing more quiescent output voltage ripple and increasing the output noise and distortion. Higher switching frequencies result in more power loss. The optimum quiescent switching frequency is approximately 600KHz to 700KHz. Refer to the Operating Specifications for recommended values. Table 1—Switching Frequency vs. VDD, Timing Capacitor and Feedback Resistor (see Figure 1) Gain (V/V) Gain (dB) RFB (kΩ) RIN (kΩ) CINT FSW VDD (V) 3.9 11.8 39 10 6.8nF 660KHz 12 8.2 18.3 82 10 3.3nF 660KHz 12 8.3 18.4 39 4.7 6.8nF 660KHz 12 12.0 21.6 120 10 2.2nF 610KHz 12 17.4 24.8 82 4.7 3.3nF 660KHz 12 25.5 28.1 120 4.7 2.2nF 610KHz 12 5.6 15.0 56 10 8.2nF 670KHz 24 8.2 18.3 82 10 5.6nF 720KHz 24 11.9 21.5 56 4.7 8.2nF 670KHz 24 12.0 21.6 120 10 4.7nF 620KHz 24 17.4 24.8 82 4.7 5.6nF 720KHz 24 25.5 28.1 120 4.7 4.7nF 620KHz 24 33.0 30.4 330 10 1.8nF 700KHz 24 Choosing the LC Filter The Inductor-Capacitor (LC) filter converts the pulse train at SW to the output voltage that drives the speaker. The characteristic frequency of the LC filter needs to be high enough to allow high frequency audio to the output, yet needs to be low enough to filter out high frequency products of the pulses from SW. The characteristic frequency of the LC filter is: LC 2 1 f0 π = The voltage ripple at the output is approximated by the equation: ⎟⎟ ⎠ ⎞ ⎜⎜ ⎝ ⎛ × ≅ SW 0 DD RIPPLE f f V V The quality factor (Q) of the LC filter is important. If this is too low, output noise will increase, if this is too high, then peaking may occur at high signal frequencies reducing the passband flatness. The circuit Q is set by the load resistance (speaker resistance, typically 4Ω or 8Ω). The Q is calculated as: |
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