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SPC560P50L3 Datasheet(PDF) 82 Page - STMicroelectronics |
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SPC560P50L3 Datasheet(HTML) 82 Page - STMicroelectronics |
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82 / 112 page ![]() Electrical characteristics SPC560P44Lx, SPC560P50Lx 82/112 Doc ID 14723 Rev 9 Equation 7 ● A second charge transfer involves also CF (that is typically bigger than the on-chip capacitance) through the resistance RL: again considering the worst case in which CP2 and CS were in parallel to CP1 (since the time constant in reality would be faster), the time constant is: Equation 8 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: Equation 9 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. Equation 10 must be respected (charge balance assuming now CS already charged at VA1): Equation 10 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. Figure 18. Spectral representation of input signal V A1 C S C P1 C P2 ++ () • V A C P1 C P2 + () • = τ 2 R L < C S C P1 C P2 ++ () • 8.5 τ 2 • 8.5 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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