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LTC2485CDD Datasheet(PDF) 22 Page - Linear Technology |
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LTC2485CDD Datasheet(HTML) 22 Page - Linear Technology |
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22 / 40 page ![]() 22 LTC2485 2485fa For a simple approximation, the source impedance RS driving an analog input pin (IN+, IN–, REF+ or REF–) can be considered to form, together with RSW and CEQ (see Figure 12), a first order passive network with a time con- stant τ = (RS + RSW) • CEQ. The converter is able to sample the input signal with better than 1ppm accuracy if the sampling period is at least 14 times greater than the input circuit time constant τ. The sampling process on the four input analog pins is quasi-independent so each time con- stant should be considered by itself and, under worst-case circumstances, the errors may add. When using the internal oscillator, the LTC2485’s front- end switched-capacitor network is clocked at 123kHz corresponding to an 8.1 µs sampling period. Thus, for settling errors of less than 1ppm, the driving source impedance should be chosen such that τ ≤ 8.1µs/14 = 580ns. When an external oscillator of frequency fEOSC is used, the sampling period is 2.5/fEOSC and, for a settling error of less than 1ppm, τ ≤ 0.178/fEOSC. Automatic Differential Input Current Cancellation In applications where the sensor output impedance is low (up to 10k Ω with no external bypass capacitor or up to 500 Ω with 0.001µF bypass), complete settling of the input occurs. In this case, no errors are introduced and direct digitization of the sensor is possible. For many applications, the sensor output impedance com- bined with external bypass capacitors produces RC time constants much greater than the 580ns required for 1ppm accuracy. For example, a 10k Ω bridge driving a 0.1µF bypass capacitor has a time constant an order of magni- tude greater than the required maximum. Historically, settling issues were solved using buffers. These buffers led to increased noise, reduced DC performance (Offset/ Drift), limited input/output swing (cannot digitize signals near ground or VCC), added system cost and increased power. The LTC2485 uses a proprietary switching algo- rithm that forces the average differential input current to zero independent of external settling errors. This allows accurate direct digitization of high impedance sensors without the need of buffers (see Figures 13 to 15). Addi- tional errors resulting from mismatched leakage currents must also be taken into account. The switching algorithm forces the average input current on the positive input (IIN+) to be equal to the average input current on the negative input (IIN–). Over the complete conversion cycle, the average differential input current (IIN+ – IIN–) is zero. While the differential input current is zero, the common mode input current (IIN++ IIN–)/2 is proportional to the difference between the common mode input voltage (VINCM) and the common mode reference voltage (VREFCM). In applications where the input common mode voltage is equal to the reference common mode voltage, as in the case of a balance bridge type application, both the differ- ential and common mode input current are zero. The accuracy of the converter is unaffected by settling errors. Mismatches in source impedances between IN+ and IN– also do not affect the accuracy. In applications where the input common mode voltage is constant but different from the reference common mode voltage, the differential input current remains zero while the common mode input current is proportional to the difference between VINCM and VREFCM. For a reference common mode of 2.5V and an input common mode of 1.5V, the common mode input current is approximately 0.74 µA (in simultaneous 50Hz/60Hz rejection mode). This common mode input current has no effect on the accuracy if the external source impedances tied to IN+ and IN– are matched. Mismatches in these source impedances lead to a fixed offset error but do not affect the linearity or full- scale reading. A 1% mismatch in 1k Ω source resistances leads to a 15ppm shift (74 µV) in offset voltage. In applications where the common mode input voltage varies as a function of input signal level (single-ended input, RTDs, half bridges, current sensors, etc.), the common mode input current varies proportionally with input voltage. For the case of balanced input impedances, the common mode input current effects are rejected by the large CMRR of the LTC2485 leading to little degradation in accuracy. Mismatches in source impedances lead to gain errors proportional to the difference between the common mode input voltage and the common mode reference voltage. 1% mismatches in 1k Ω source resistances lead to worst-case gain errors on the order of 15ppm or 1LSB (for 1V differences in reference and input common mode APPLICATIO S I FOR ATIO |
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