SBAA275A June 2018 – March 2023 ADS1120 , ADS112C04 , ADS112U04 , ADS1147 , ADS1148 , ADS114S06 , ADS114S06B , ADS114S08 , ADS114S08B , ADS1220 , ADS122C04 , ADS122U04 , ADS1247 , ADS1248 , ADS124S06 , ADS124S08 , ADS125H02 , ADS1260 , ADS1261 , ADS1262 , ADS1263
Many precision ADCs used for RTD measurement will have programmable excitation current sources (IDACs) in several magnitudes. A precision ADC device may have a matched pair of IDACs used for excitation. These IDACs can be set to currents of 10, 50, 100, 250, 500, 750, 1000, 1500, and 2000 µA. Excitation currents are used to drive both the RTD, the reference resistance and biasing resistors for some designs.
For the best noise performance, maximize the excitation current used for the RTD and reference resistance excitation. However, most excitation currents should be kept lower than 1 mA because of self heating. Because there is current running through the RTD, the RTD itself will dissipate power through heat. This self heating will cause an error in the measurement. The change in temperature (ΔT) is determined by the power dissipation of the RTD divided by the self-heating coefficient E, in mW/°C. This change in temperature becomes a temperature measurement error and is shown in Equation 14.
The typical range of RTD self-heating coefficients is 2.5 mW/°C for small, thin-film elements and 65 mW/°C for larger, wire-wound elements. With 1-mA excitation at the maximum RTD resistance value and a larger self-heating coefficient, the power dissipation in the RTD is less than 0.4 mW and will keep the measurement errors due to self-heating to less than 0.01°C. Self-heating coefficients will vary with RTD construction and the measurement medium (in air or in water, for example). Consult the RTD manufacturer data sheet for sensor characteristics.
Referring back to Figure 1-4, this topology uses a single IDAC current source. Other topologies may use matched sources to for lead current calculation.