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TS4962M 数据表(PDF) 29 Page - STMicroelectronics |
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TS4962M 数据表(HTML) 29 Page - STMicroelectronics |
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29 / 41 page ![]() TS4962M Application information 29/41 5.3 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 Vicm limitation in the input stage (see Table 2: Operating conditions on page 3), the common mode feedback loop can ensure 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 150k Ω resistor, it’s also important to check Vicm in these conditions: If the result of Vicm calculation is not in the previous range, input coupling capacitors must be used (with VCC from 2.4V to 2.5V, input coupling capacitors are mandatory). For example: With VCC =3V, Rin = 150k and VIC = 2.5V, we typically find Vicm = 2V and this is lower than 3V - 0.8V = 2.2V. With 136.5k Ωwe find 1.97V, and with 163.5kΩwe have 2.02V. So, no input coupling capacitors are required. 5.4 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 -3dB 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 × 2V IC × 150k Ω × + 2R in 150k Ω + () × ------------------------------------------------------------------------------ (V) = V IC In + In - + 2 --------------------- (V) = 0.5V V icm V CC 0.8V – ≤≤ V CC R in × 2V IC × 136.5k Ω × + 2R in 136.5k Ω + () × ----------------------------------------------------------------------------------- V icm V CC R in × 2V IC × 163.5k Ω × + 2R 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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