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LM4849 датащи(PDF) 18 Page - National Semiconductor (TI) |
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LM4849 датащи(HTML) 18 Page - National Semiconductor (TI) |
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18 / 19 page ![]() Application Information (Continued) supply voltage must also not create a situation that violates of maximum power dissipation as explained above in the Power Dissipation section. After satisfying the LM4849’s power dissipation require- ments, the minimum differential gain needed to achieve 1W dissipation in an 8 Ω load is found using Equation (13). (11) Thus, a minimum overall gain of 2.83 allows the LM4849’s to reach full output swing and maintain low noise and THD+N performance. The last step in this design example is setting the amplifier’s −3dB frequency bandwidth. To achieve the desired ±0.25dB pass band magnitude variation limit, the low frequency re- sponse must extend to at least one-fifth the lower bandwidth limit and the high frequency response must extend to at least five times the upper bandwidth limit. The gain variation for both response limits is 0.17dB, well within the ±0.25dB desired limit. The results are an f L = 100Hz/5 = 20Hz (12) and an f H = 20kHzx5= 100kHz (13) As mentioned in the Selecting Proper External Compo- nents section, R i (Right & Left) and Ci (Right & Left) create a highpass filter that sets the amplifier’s lower bandpass frequency limit. Find the coupling capacitor’s value using Equation (17). C i ≥ 1/(2πR ifL) (14) The result is 1/(2 π*20kΩ*20Hz) = 0.397µF (15) Use a 0.39µF capacitor, the closest standard value. The product of the desired high frequency cutoff (100kHz in this example) and the differential gain A VD, determines the upper passband response limit. With A VD = 3 and fH = 100kHz, the closed-loop gain bandwidth product (GBWP) is 300kHz. This is less than the LM4849’s 3.5MHz GBWP. With this margin, the amplifier can be used in designs that require more differential gain while avoiding performance,restricting bandwidth limitations. www.national.com 18 |
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