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LM4953SD датащи(PDF) 7 Page - National Semiconductor (TI) |
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LM4953SD датащи(HTML) 7 Page - National Semiconductor (TI) |
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7 / 11 page ![]() Typical Performance Characteristics (Continued) Supply Current vs Supply Voltage Z L = 2µF+30 Ω 20142127 Application Information ELIMINATING THE OUTPUT COUPLING CAPACITOR The LM4953 features a low noise inverting charge pump that generates an internal negative supply voltage. This allows the outputs of the LM4953 to be biased about GND instead of a nominal DC voltage, like traditional headphone amplifi- ers. Because there is no DC component, the large DC blocking capacitors (typically 220µF) are not necessary. The coupling capacitors are replaced by two, small ceramic charge pump capacitors, saving board space and cost. Eliminating the output coupling capacitors also improves low frequency response. In traditional headphone amplifiers, the headphone impedance and the output capacitor form a high pass filter that not only blocks the DC component of the output, but also attenuates low frequencies, impacting the bass response. Because the LM4953 does not require the output coupling capacitors, the low frequency response of the device is not degraded by external components. In addition to eliminating the output coupling capacitors, the ground referenced output nearly doubles the available dy- namic range of the LM4953 when compared to a traditional headphone amplifier operating from the same supply volt- age. BRIDGE CONFIGURATION EXPLANATION The Audio Amplifier portion of the LM4953has two internal amplifiers allowing different amplifier configurations. The first amplifier’s gain is externally configurable, whereas the sec- ond amplifier is internally fixed in a unity-gain, inverting configuration. The closed-loop gain of the first amplifier is set by selecting the ratio of Rf to Ri while the second amplifier’s gain is fixed by the two internal 20k Ω resistors. Figure 1 shows that the output of amplifier one serves as the input to amplifier two. This results in both amplifiers producing sig- nals identical in magnitude, but out of phase by 180˚. Con- sequently, the differential gain for the Audio Amplifier is A VD = 2 *(Rf/Ri) By driving the load differentially through outputs OUT A and OUT B, an amplifier configuration commonly referred to as “bridged mode” is established. Bridged mode operation is different from the classic single-ended amplifier configura- tion where one side of the load is connected to ground. A bridge amplifier design has a few distinct advantages over the single-ended configuration. It provides differential drive to the load, thus doubling the output swing for a specified supply voltage. Four times the output power is possible as compared to a single-ended amplifier under the same con- ditions. This increase in attainable output power assumes that the amplifier is not current limited or clipped. In order to choose an amplifier’s closed-loop gain without causing ex- cessive clipping, please refer to the Audio Power Amplifier Design section. The bridge configuration also creates a second advantage over single-ended amplifiers. Since the differential outputs, OUT A and OUT B, are biased at half-supply, no net DC voltage exists across the load. This eliminates the need for an output coupling capacitor which is required in a single supply, single-ended amplifier configuration. Without an out- put coupling capacitor, the half-supply bias across the load would result in both increased internal IC power dissipation and also possible loudspeaker damage. OUTPUT TRANSIENT (’CLICK AND POPS’) ELIMINATED The LM4953 contains advanced circuitry that virtually elimi- nates output transients (’clicks and pops’). This circuitry prevents all traces of transients when the supply voltage is first applied or when the part resumes operation after coming out of shutdown mode. 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 π2Z L) (1) www.national.com 7 |
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