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ST10F271 数据表(PDF) 138 Page - STMicroelectronics |
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ST10F271 数据表(HTML) 138 Page - STMicroelectronics |
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138 / 173 page ![]() Electrical characteristics ST10F271 138/173 and CS were in parallel to CP1 (since the time constant in reality would be faster), the time constant is: In this case, the time constant depends on the external circuit: in particular imposing that the transient is completed well before the end of sampling time TS, a constraints on RL sizing is obtained: Of course, RL shall be sized also according to the current limitation constraints, in combination with RS (source impedance) and RF (filter resistance). Being CF definitively bigger than CP1, CP2 and CS, then the final voltage VA2 (at the end of the charge transfer transient) will be much higher than VA1. The following equation must be respected (charge balance assuming now CS already charged at VA1): The two transients above are not influenced by the voltage source that, due to the presence of the RFCF filter, is not able to provide the extra charge to compensate the voltage drop on CS with respect to the ideal source VA; the time constant RFCF of the filter is very high with respect to the sampling time (TS). The filter is typically designed to act as anti-aliasing (see Figure 42). Calling f0 the bandwidth of the source signal (and as a consequence the cut-off frequency of the anti-aliasing filter, fF), according to Nyquist theorem the conversion rate fC must be at least 2f0; it means that the constant time of the filter is greater than or at least equal to twice the conversion period (TC). Again the conversion period TC is longer than the sampling time TS, which is just a portion of it, even when fixed channel continuous conversion mode is selected (fastest conversion rate at a specific channel): in conclusion it is evident that the time constant of the filter RFCF is definitively much higher than the sampling time TS, so the charge level on CS cannot be modified by the analog signal source during the time in which the sampling switch is closed. Figure 42. Anti-aliasing filter and conversion rate The considerations above lead to impose new constraints to the external circuit, to reduce the accuracy error due to the voltage drop on CS; from the two charge balance equations τ 2 R L < C S C P1 C P2 ++ () ⋅ 10 τ 2 ⋅ 10 R ⋅ L = C S C P1 C P2 ++ () T S ≤ ⋅ V A2 C S C P1 C P2 C F +++ () ⋅ V A C F ⋅ V A1 + C P1 C P2 +C S + () ⋅ = f0 f Analog Source Bandwidth (VA) f0 f Sampled Signal Spectrum (fC = conversion Rate) fC f Anti-Aliasing Filter (fF = RC Filter pole) fF 2 f0 ≤ fC (Nyquist) fF = f0 (Anti-aliasing Filtering Condition) TC ≤ 2 RFCF (Conversion Rate vs. Filter Pole) Noise |
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