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LTC2439-1 Datasheet(PDF) 25 Page - Linear Technology |
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LTC2439-1 Datasheet(HTML) 25 Page - Linear Technology |
25 / 28 page ![]() LTC2439-1 25 24391f impedance for the REF+ and REF– pins does not help the gain or the INL error. The user is thus advised to minimize the combined source impedance driving the REF+ and REF– pins rather than to try to match it. The magnitude of the dynamic reference current depends upon the size of the very stable internal sampling capaci- tors and upon the accuracy of the converter sampling clock. The accuracy of the internal clock over the entire temperature and power supply range is typical better than 0.5%. Such a specification can also be easily achieved by an external clock. When relatively stable resistors (50ppm/ °C) are used for the external source impedance seen by REF+ and REF–, the expected drift of the dynamic current gain error will be insignificant (about 1% of its value over the entire temperature and voltage range). Even for the most stringent applications a one-time calibration operation may be sufficient. In addition to the reference sampling charge, the reference pins ESD protection diodes have a temperature dependent leakage current. This leakage current, nominally 1nA ( ±10nA max), results in a small gain error. A 100Ω source resistance will create a 0.05 µV typical and 0.5µV maxi- mum full-scale error. Output Data Rate When using its internal oscillator, the LTC2439-1 can produce up to 6.8 readings per second. The actual output data rate will depend upon the length of the sleep and data output phases which are controlled by the user and which can be made insignificantly short. When operated with an external conversion clock (FO connected to an external oscillator), the LTC2439-1 output data rate can be in- creased as desired. The duration of the conversion phase is 20510/fEOSC. If fEOSC = 139,800Hz, the converter be- haves as if the internal oscillator is used with simultaneous 50Hz/60Hz. There is no significant difference in the LTC2439-1 performance between these two operation modes. An increase in fEOSC over the nominal 139,800Hz will translate into a proportional increase in the maximum output data rate. This substantial advantage is neverthe- less accompanied by three potential effects, which must be carefully considered. RSOURCE (Ω) 0 100 200 300 400 500 600 700 800 900 1000 24361 F21 0 6 11 17 22 30 VCC = 5V REF+ = 5V REF– = GND IN+ = 3.75V IN – = 1.25V FO = GND TA = 25°C CREF = 0.01µF CREF = 0.1µF CREF = 1µF, 10µF RSOURCE (Ω) 0 100 200 300 400 500 600 700 800 900 1000 24361 F22 30 22 17 11 6 0 VCC = 5V REF+ = 5V REF– = GND IN+ = 1.25V IN – = 3.75V FO = GND TA = 25°C CREF = 0.01µF CREF = 0.1µF CREF = 1µF, 10µF VINDIF/VREFDIF –0.5 –0.4–0.3–0.2–0.1 0 0.1 0.2 0.3 0.4 0.5 1 0 –1 VCC = 5V REF+ = 5V REF– = GND VINCM = 0.5 • (IN + + IN–) = 2.5V FO = GND CREF = 10µF TA = 25°C RSOURCE = 1000Ω 24361 F23 Figure 21. +FS Error vs RSOURCE at REF+ and REF– (Large CREF) Figure 22. –FS Error vs RSOURCE at REF+ and REF– (Large CREF) Figure 23. INL vs Differential Input Voltage (VIN = IN + – IN–) and Reference Source Resistance (RSOURCE at REF+ and REF– for Large CREF Values (CREF ≥ 1µF) APPLICATIO S I FOR ATIO |
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