SBAA532A February 2022 – March 2024 ADS1119 , ADS1120 , ADS1120-Q1 , ADS112C04 , ADS112U04 , ADS1130 , ADS1131 , ADS114S06 , ADS114S06B , ADS114S08 , ADS114S08B , ADS1158 , ADS1219 , ADS1220 , ADS122C04 , ADS122U04 , ADS1230 , ADS1231 , ADS1232 , ADS1234 , ADS1235 , ADS1235-Q1 , ADS124S06 , ADS124S08 , ADS1250 , ADS1251 , ADS1252 , ADS1253 , ADS1254 , ADS1255 , ADS1256 , ADS1257 , ADS1258 , ADS1258-EP , ADS1259 , ADS1259-Q1 , ADS125H01 , ADS125H02 , ADS1260 , ADS1260-Q1 , ADS1261 , ADS1261-Q1 , ADS1262 , ADS1263 , ADS127L01 , ADS130E08 , ADS131A02 , ADS131A04 , ADS131E04 , ADS131E06 , ADS131E08 , ADS131E08S , ADS131M02 , ADS131M03 , ADS131M04 , ADS131M06 , ADS131M08
In addition to low noise, bridge measurement systems typically require high accuracy. As discussed in Section 4.4, AC excitation is one solution to remove offset error from a bridge measurement. This method is similar to amplifier chopping where the input channel is swapped between the positive and negative inputs. However, AC excitation swaps the polarity of VEXCITATION between the top (Phase 1) and bottom (Phase 2) of the bridge. The ADC measures the output of the bridge during both phases, subtracts the Phase 2 measurement from the Phase 1 measurement, and averages the result. This process cancels any systemic offsets after the bridge that can be caused by parasitic thermocouples or external amplifier offsets for example. This technique produces a measured result that is just the bridge output voltage.
Figure 5-9 shows an ADC bridge measurement during Phase 1 where VEXCITATION is at the top of the bridge, the bottom of the bridge is grounded, and an offset (VOS) is shown as a source voltage between the bridge and the ADC.
Equation 28 calculates the voltage measured by the ADC during Phase 1:
After the first ADC measurement completes, Phase 2 swaps the bridge polarity such that VEXCITATION is routed to the bottom of the bridge and the top of the bridge is grounded. This swapping inverts the output voltage while maintaining the polarity of VOS. The Phase 2 configuration is shown in Figure 5-10.
Equation 29 calculates the voltage measured by the ADC during Phase 2:
Subtracting the result of Equation 29 from Equation 28 and dividing by two yields Equation 30:
Ultimately, Equation 30 shows that VOS cancels out and the final result is just VOUT, thereby removing the total offset error after the bridge. However, it is important to note that systemic offsets that occur inside the bridge or before the chopping circuitry are not removed by AC excitation. Instead, use calibration to remove the inherent bridge offset.
Implementing AC excitation requires external transistors, gate drivers, or other switches to swap the bridge excitation voltage polarity. General purpose outputs (GPOs) from the ADC or host typically control the switching, and should be implemented with non-overlapping clocks to prevent bridge cross-conduction during voltage reversal.
Several TI precision ADCs are designed to implement AC excitation. The ADS1235 has specific pins to control external switches that swap the bridge polarity. For more information about implementing AC excitation for bridge measurements, see the Reduce Bridge Measurement Offset and Drift Using the AC Excitation Mode application note.