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LTC2436-1IGN датащи(PDF) 21 Page - Linear Technology |
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LTC2436-1IGN датащи(HTML) 21 Page - Linear Technology |
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21 / 28 page ![]() LTC2436-1 21 24361f by Figures 14 and 15. For simplicity, two distinct situa- tions 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 filtering 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 LTC2436-1 can maintain its accuracy while operating with relative large values of source resistance as shown in Figure 16. +FS Error vs RSOURCE at IN+ or IN– (Large CIN) Figure 17. –FS Error vs RSOURCE at IN+ or IN– (Large CIN) APPLICATIO S I FOR ATIO RSOURCE (Ω) 0 100 200 300 400 500 600 700 800 900 1000 24361 F16 20 16 12 8 4 0 VCC = 5V REF+ = 5V REF – = GND IN+ = 3.75V IN– = 1.25V FO = GND TA = 25°C CIN = 0.01µF CIN = 0.1µF CIN = 1µF, 10µF RSOURCE (Ω) 0 100 200 300 400 500 600 700 800 900 1000 24361 F17 0 –4 –8 –12 –16 –20 VCC = 5V REF+ = 5V REF – = GND IN+ = 1.25V IN– = 3.75V FO = GND TA = 25°C CIN = 0.01µF CIN = 0.1µF CIN = 1µF, 10µF Figure 15. –FS Error vs RSOURCE at IN + or IN– (Small CIN) RSOURCE (Ω) 1 10 100 1k 10k 100k 24361 F15 0 –3 –2 –1 VCC = 5V REF+ = 5V REF – = GND IN+ = GND IN– = 2.5V FO = GND TA = 25°C CIN = 0.01µF CIN = 0.001µF CIN = 100pF CIN = 0pF Figures 14 and 15. These measured results may be slightly different from the first order approximation suggested earlier because they include 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 imped- ance 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 50Hz/60Hz notch), the typical differential input resistance is 2M Ω which will generate a gain error of approximately 1LSB at full scale for each 60 Ω of source resistance driving IN+ or IN–. When FO is driven by an external oscillator with a fre- quency fEOSC (external conversion clock operation), the typical differential input resistance is 0.28 • 1012/fEOSCΩ and each ohm of source resistance driving IN+ or IN– will result in 1.11 • 10–7 • fEOSCLSB gain error at full scale. The effect of the source resistance on the two input pins is additive with respect to this gain error. The typical +FS and –FS errors as a function of the sum of the source resis- tance seen by IN+ and IN– for large values of CIN are shown in Figures 16 and 17. |
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