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LM4876MM Datasheet(PDF) 8 Page - Texas Instruments |
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LM4876MM Datasheet(HTML) 8 Page - Texas Instruments |
8 / 19 page LM4876 SNAS054E – FEBRUARY 2000 – REVISED MAY 2013 www.ti.com APPLICATION INFORMATION BRIDGE CONFIGURATION EXPLANATION As shown in Figure 1, the LM4876 consists of two operational amplifiers. External resistors Rf and Ri set the closed-loop gain of Amp1, whereas two internal 40k Ω resistors set Amp2's gain at -1. The LM4876 drives a load, such as a speaker, connected between the two amplifier outputs, Vo1 and Vo2 . Figure 1 shows that the Amp1 output serves as the Amp2 input, which results in both amplifiers producing signals identical in magnitude, but 180° out of phase. Taking advantage of this phase difference, a load is placed between Vo1 and Vo2 and driven differentially (commonly referred to as "bridge mode"). This results in a differential gain of AVD = 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 power assumes that the amplifier is not current limited or that 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 AMPLIFIER DESIGN section. Another advantage of the differential bridge output is no net DC voltage across the load. This results from biasing Vo1 and Vo2 at half-supply. This eliminates the coupling capacitor that single supply, single-ended amplifiers require. Eliminating an output coupling capacitor in a single-ended configuration forces a single-supply amplifier's half-supply bias voltage 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 output load. PDMAX = (VDD) 2 /(2π2 R L) Single-Ended (2) However, a direct consequence of the increased power delivered to the load by a bridge amplifier is higher internal power dissipation for the same conditions. The LM4876 has two operational amplifiers in one package and the maximum internal power dissipation is four times that of a single-ended amplifier. Equation 3 states the maximum power dissipation for a bridge amplifier. However, even with this substantial increase in power dissipation, the LM4876 does not require heatsinking. From Equation 3, assuming a 5V power supply and an 8 Ω load, the maximum power dissipation point is 633mW. PDMAX = 4*(VDD) 2 /(2π2 R L ) Bridge Mode (3) The maximum power dissipation point given by Equation 3 must not exceed the power dissipation given by Equation 4: PDMAX = (TJMAX -TA) /θJA (4) The LM4876's TJMAX = 150°C. In the D package, the LM4876's θJA is 140°C/W. At any given ambient temperature TA, use Equation 4 to find the maximum internal power dissipation supported by the IC packaging. Rearranging Equation 4 results in Equation 5. This equation gives the maximum ambient temperature that still allows maximum power dissipation without violating the LM4876's maximum junction temperature. TA = TJMAX - PDMAX θJA (5) For a typical application with a 5V power supply and an 8W load, the maximum ambient temperature that allows maximum power dissipation without exceeding the maximum junction temperature is approximately 61°C. TJMAX = PDMAX θJA + TA (6) 8 Submit Documentation Feedback Copyright © 2000–2013, Texas Instruments Incorporated Product Folder Links: LM4876 |
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