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EUA6412 Datasheet(PDF) 13 Page - Eutech Microelectronics Inc |
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EUA6412 Datasheet(HTML) 13 Page - Eutech Microelectronics Inc |
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13 / 18 page ![]() EUA6412 DS6412 Ver 1.0 Dec. 2006 13 Application Information Gain Setting The gain of the EUA6412 is set by two input terminals, Gain0 and Gain1.The gains listed in Table 1 are realized by changing the taps on the input resistors inside the amplifier. Table 1.Gain Setting GAIN0 GAIN1 BTL SE/ AV(inv) ZI 0 0 0 6dB 90kΩ 0 1 0 10dB 70kΩ 1 0 0 15.6dB 45kΩ 1 1 0 21.6dB 25kΩ X X 1 4.1dB Input Resistance Each gain setting is achieved by varying the input resistance of the amplifier, which can range from its smallest value to over 6 times that value. As a results, if a single capacitor is used in the input high pass filter, the –3 dB or cut off frequency will also change by over 6 times. If an additional resistor is connected from the input pin of the amplifier to ground, as shown in the figure below, the variation of the cut-off frequency will be much reduced. The-3dB frequency can be calculated using equation 1: f-3dB = ---------------------- (1) If the filter must be more accurate, the value of the capacitor should be increased while the value of the resistor to ground should be decreased. In addition, the order of the filter could be increased. Input Capacitor, Ci In the typical application an input capacitor, Ci, is required to allow the amplifier to bias the input signal to the proper dc level for optimum operation. In this case, Ci and the input impedance of the amplifier, Zi, from a high-pass filter with the corner frequency determined in equation 2. fc(highpass)= i i C Z 2 1 π -----------------(2) The value of Ci is important to consider as it directly affects the bass (low frequency) performance of the circuit. Consider the example where Zi is 710kΩ and the specification calls for a flat bass response down to 40Hz. Equation 2 is reconfigured as equation 3. Ci = C f Z 2 1 i π ----------------------------- (3 ) In this example, Ci is 5.6nF so one would likely choose a value in the range of 5.6nF to 1µF. A further consideration for this capacitor is the leakage path from the input source through the input network (Ci) and the feedback network to the load. This leakage current creates a dc offset voltage at the input to the amplifier that reduces useful headroom, especially in high gain applications. For this reason a low- leakage tantalum or ceramic capacitor is the best choice. When polarized capacitors are used, the positive side of the capacitor should face the amplifier input in most applications as the dc level there is held at VDD/2, which is likely higher than the source dc level. Note that it is important to confirm the capacitor polarity in the application. ) i R || (R C 2 1 π |
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