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TS4962 датащи(PDF) 31 Page - STMicroelectronics |
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TS4962 датащи(HTML) 31 Page - STMicroelectronics |
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31 / 44 page ![]() DocID10968 Rev 9 31/44 TS4962 Application information 44 4.3 Common-mode feedback loop limitations As explained previously, the common-mode feedback loop allows the output DC bias voltage to be averaged at VCC/2 for any DC common-mode bias input voltage. However, due to a Vicm limitation in the input stage (see Table 3: Operating conditions on page 4 ), the common-mode feedback loop can play its role only within a defined range. This range depends upon the values of VCC and Rin (AVdiff). To have a good estimation of the Vicm value, we can apply this formula (no tolerance on Rin): with And the result of the calculation must be in the range: Due to the +/-9% tolerance on the 150 k Ω resistor, it is also important to check V icm in these conditions. If the result of the Vicm calculation is not in the previous range, input coupling capacitors must be used. With VCC between 2.4 and 2.5 V, input coupling capacitors are mandatory. For example: With VCC = 3 V, Rin = 150 k and VIC = 2.5 V, we typically find Vicm = 2 V, which is lower than 3 V-0.8 V = 2.2 V. With 136.5 k Ω we find 1.97 V and with 163.5 kΩ we have 2.02 V. Therefore, no input coupling capacitors are required. 4.4 Low frequency response If a low frequency bandwidth limitation is requested, it is possible to use input coupling capacitors. In the low frequency region, Cin (input coupling capacitor) starts to have an effect. Cin forms, with Rin, a first order high-pass filter with a -3 dB cut-off frequency. So, for a desired cut-off frequency we can calculate Cin, with Rin in Ω and FCL in Hz. V icm V CC R in × 2 V IC × 150k Ω × + 2 R in 150k Ω + ( ) × ---------------------------------------------------------------------------- (V) = V IC In + In - + 2 --------------------- (V) = 0.5V V icm V CC 0.8V – ≤ ≤ V CC R in × 2 V IC × 136.5k Ω × + 2 R in 136.5k Ω + ( ) × --------------------------------------------------------------------------------- V icm V CC R in × 2 V IC × 163.5k Ω × + 2 R in 163.5k Ω + ( ) × --------------------------------------------------------------------------------- ≤ ≤ F CL 1 2 π R in × C in × ------------------------------------ (Hz) = C in 1 2 π R in × F CL × -------------------------------------- (F) = |
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