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LM4818 Datasheet(PDF) 9 Page - National Semiconductor (TI) |
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LM4818 Datasheet(HTML) 9 Page - National Semiconductor (TI) |
9 / 16 page Application Information BRIDGE CONFIGURATION EXPLANATION As shown in Figure 1, the LM4818 consist of two operational amplifiers. External resistors, R i and RF set the closed-loop gain of the first amplifier (and the amplifier overall), whereas two internal 20k Ω resistors set the second amplifier’s gain at -1. The LM4818 is typically used to drive a speaker con- nected between the two amplifier outputs. Figure 1 shows that the output of Amp1 servers as the input to Amp2, which results in both amplifiers producing signals identical in magnitude but 180˚ out of phase. Taking advan- tage of this phase difference, a load is placed between V 01 and V 02 and driven differentially (commonly referred to as ’bridge mode’). This results in a differential gain of A VD= 2 *(Rf/Ri) (1) Bridge mode is different from single-ended amplifiers that drive loads connected between a single amplifier’s output and ground. For a given supply voltage, bridge mode has a distinct advantage over the single-ended configuration: its differential output doubles the voltage swing across the load. This results in four times the output power when compared to a single-ended amplifier under the same conditions. This increase in attainable output assumes that the amplifier is not current limited or the output signal is not clipped. To ensure minimum output signal clipping when choosing an amplifier’s closed-loop gain, refer to the Audio Power Am- plifier Design Example section. Another advantage of the differential bridge output is no net DC voltage across the load. This results from biasing V 01 and V 02 at half-supply. This eliminates the coupling capacitor that single supply, single-ended amplifiers require. Eliminat- ing an output coupling capacitor in a single-ended configu- ration forces a single supply amplifier’s half-supply bias volt- age across the load. The current flow created by the half- supply bias voltage increases internal IC power dissipation and may permanently damage loads such as speakers. POWER DISSIPATION Power dissipation is a major concern when designing a successful bridged or single-ended amplifier. Equation (2) states the maximum power dissipation point for a single- ended amplifier operating at a given supply voltage and driving a specified load. P DMAX =(VDD) 2 /(2 π2R L ) (W) Single-ended (2) However, a direct consequence of the increased power de- livered to the load by a bridged amplifier is an increase in the internal power dissipation point for a bridge amplifier oper- ating at the same given conditions. Equation (3) states the maximum power dissipation point for a bridged amplifier operating at a given supply voltage and driving a specified load. P DMAX = 4(VDD) 2/(2 π2 R L ) (W) Bridge Mode (3) The LM4818 has two operational amplifiers in one package and the maximum internal power dissipation is four times that of a single-ended amplifier. However, even with this substantial increase in power dissipation, the LM4818 does not require heatsinking. From Equation (3), assuming a 5V power supply and an 8 Ω load, the maximum power dissipa- tion point is 633mW. The maximum power dissipation point obtained from Equation (3) must not exceed the power dis- sipation predicted by Equation (4): P DMAX =(TJMAX -TA)/θJA (W) (4) For the M08A package, θ JA = 170˚C/W and TJMAX = 150˚C for the LM4818. For a given ambient temperature, T A, Equa- tion (4) can be used to find the maximum internal power dissipation supported by the IC packaging. If the result of Equation (3) is greater than the result of Equation (4), then decrease the supply voltage, increase the load impedance, or reduce the ambient temperature. For a typical application using the M08A packaged LM4818 with a 5V power supply and an 8 Ω load, the maximum ambient temperature that does not violate the maximum junction temperature is ap- proximately 42˚C. It is assumed that a device is a surface mount part operating around the maximum power dissipation point. The assumption that the device is operating around the maximum power dissipation point is incorrect for an 8 Ω load. The maximum power dissipation point occurs when the output power is equal to the maximum power dissipation or 50% efficiency. The LM4818 is not capable of the output power level (633mW) required to operate at the maximum power dissipation point for an 8 Ω load. To find the maximum power dissipation, the graph Power Dissipation vs. Output Power must be used. From the graph, the maximum power dissipation for an 8 Ω load and a 5V supply is approximately 575mW. Substituting this value back into equation (4) for P DMAX and using θJA = 170˚C/W for the M08A package, the maximum ambient temperature is 52˚C. Refer to the Typical Performance Characteristics curves for power dissipation information for lower output powers and maximum power dissipation for each package at a given ambient tempera- ture. POWER SUPPLY BYPASSING As with any power amplifier, proper supply bypassing is critical for low noise performance and high power supply rejection. The capacitors connected to the bypass and power supply pins should be placed as close to the LM4818 as possible. The capacitor connected between the bypass pin and ground improves the internal bias voltage’s stability, producing improved PSRR. The improvements to PSRR increase as the bypass pin capacitor value increases. Typi- cal applications employ a 5V regulator with 10µF and 0.1µF filter capacitors that aid in supply stability. Their presence, however, does not eliminate the need for bypassing the supply nodes of the LM4818. The selection of bypass ca- pacitor values, especially C B , depends on desired PSRR requirements, click and pop performance as explained in the section, Proper Selection of External Components, as well as system cost and size constraints. SHUTDOWN FUNCTION The voltage applied to the LM4818’s SHUTDOWN pin con- trols the shutdown function. Activate micro-power shutdown by applying V DD to the SHUTDOWN pin. When active, the LM4818’s micro-power shutdown feature turns off the ampli- fier’s bias circuitry, reducing the supply current. The logic threshold is typically 1/2V DD. The low 0.7µA typical shut- down current is achieved by applying a voltage that is as near as V DD as possible to the SHUTDOWN pin. A voltage that is less than V DD may increase the shutdown current. Avoid intermittent or unexpected micro-power shutdown by ensuring that the SHUTDOWN pin is not left floating but connected to either V DD or GND. There are a few ways to activate micro-power shutdown. These included using a single-pole, single-throw switch, a microcontroller, or a microprocessor. When using a switch, connect an external 10k Ω to 100kΩ pull-up resistor between the SHUTDOWN pin and V DD. Connect the switch between the SHUTDOWN pin and ground. Select normal amplifier www.national.com 9 |
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