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LTC2430IGN Datasheet(PDF) 23 Page - Linear Technology |
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LTC2430IGN Datasheet(HTML) 23 Page - Linear Technology |
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23 / 40 page ![]() LTC2430/LTC2431 23 24301f sampling charge transfers when integrated over a sub- stantial time period (longer than 64 internal clock cycles). The effect of this input dynamic current can be analyzed using the test circuit of Figure 12. The CPAR capacitor includes the LTC2430/LTC2431 pin capacitance (5pF typi- cal) plus the capacitance of the test fixture used to obtain the results shown in Figures 13 and 14. A careful imple- mentation can bring the total input capacitance (CIN + CPAR) closer to 5pF thus achieving better performance than the one predicted by Figures 13 and 14. For simplic- ity, two distinct situations can be considered. For relatively small values of input capacitance (CIN < 0.01 µF), the voltage on the sampling capacitor settles almost completely and relatively large values for the source impedance result in only small errors. Such values for CIN will deteriorate the converter offset and gain performance without significant benefits of signal filter- ing and the user is advised to avoid them. Nevertheless, when small values of CIN are unavoidably present as parasitics of input multiplexers, wires, connectors or sensors, the LTC2430 or LTC2431 can maintain its excep- tional accuracy while operating with relative large values of source resistance as shown in Figures 13 and 14. These measured results may be slightly different from the first order approximation suggested earlier because they in- clude the effect of the actual second order input network together with the nonlinear settling process of the input amplifiers. For small CIN values, the settling on IN+ and IN– occurs almost independently and there is little benefit in trying to match the source impedance for the two pins. Larger values of input capacitors (CIN > 0.01µF) may be required in certain configurations for antialiasing or gen- eral input signal filtering. Such capacitors will average the input sampling charge and the external source resistance will see a quasi constant input differential impedance. When FO = LOW (internal oscillator and 60Hz notch), the typical differential input resistance is 21.6M Ω which will generate a gain error of approximately 0.023ppm for each ohm of source resistance driving IN+ or IN–. When FO = HIGH (internal oscillator and 50Hz notch), the typical differential input resistance is 26M Ω which will generate a gain error of approximately 0.019ppm for each ohm of source resistance driving IN+ or IN–. When FO is driven by an external oscillator with a frequency fEOSC (external conversion clock operation), the typical differential input resistance is 3.3 • 1012/fEOSCΩ and each ohm of source resistance driving IN+ or IN– will result in 0.15 • 10–6 • fEOSCppm gain error. The effect of the source resistance on the two input pins is additive with respect to this gain error. APPLICATIO S I FOR ATIO Figure 12. An RC Network at IN+ and IN– Figure 13. +FS Error vs RSOURCE at IN+ or IN– (Small CIN) Figure 14. –FS Error vs RSOURCE at IN + or IN– (Small CIN) CIN 2431 F12 VINCM + 0.5VIN RSOURCE CPAR ≅20pF CIN VINCM – 0.5VIN RSOURCE CPAR ≅20pF IN+ IN – LTC2430/ LTC2431 RSOURCE (Ω) 1 10 100 1k 10k 100k 2431 F13 50 40 30 20 10 0 –10 VCC = 5V VREF+ = 5V VREF– = GND VIN+ = 3.75V VIN– = 1.25V FO = GND TA = 25°C CIN = 0.01µF CIN = 0pF CIN = 0.001µF CIN = 100pF RSOURCE (Ω) 1 –50 –40 –30 –20 –10 0 10 10 100 1k 10k 2431 F14 100k VCC = 5V VREF+ = 5V VREF– = GND VIN+ = 1.25V VIN– = 3.75V FO = GND TA = 25°C CIN = 0.01µF CIN = 0pF CIN = 0.001µF CIN = 100pF |
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