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 systems where long lead wires are used to connect the bridge to the terminal block, wire impedance can contribute a small voltage drop between the terminal block and the bridge itself. Under these circumstances, VEXCITATION+ ≠ VSENSE+ and VEXCITATION- ≠ VSENSE- in Figure 6-2. Therefore, simply shorting VEXCITATION to VREF similar to Figure 6-1 causes a voltage mismatch between the REFP and REFN pins compared the actual voltage across the bridge, resulting in a gain error. The six-wire resistive bridge accounts for this voltage drop by including two sense lines in addition to the signal and excitation leads. These additional wires route the actual voltage seen at the top and bottom of the bridge to the REFP and REFN pins on the ADC, respectively.
The unipolar excitation voltage applied to the bridge, VEXCITATION, is used as the ADC supply voltage (AVDD) but not as the ADC reference voltage, VREF. Instead, the separate sense lines result in VREF = VSENSE+ – VSENSE-, which is slightly smaller compared to VEXCITATION but still ratiometric to the input voltage, VIN. Small variations in the bridge resistance due to tension or compression cause the differential bridge output voltage to change. The PGA integrated into the ADC gains up this low-level signal to reduce system noise and utilize more of the ADC full-scale range (FSR). The ADC samples and converts this amplified voltage against VREF, which has a ratiometric relationship to VEXCITATION. The excitation source noise and drift are seen equally in both VIN and VREF in a ratiometric reference configuration, effectively removing these errors from the ADC output code.
A six-wire resistive bridge measurement with a ratiometric reference and a unipolar, low-voltage (≤ 5 V) supply requires:
First, identify the maximum differential output voltage of the bridge, VOUT(Bridge Max), using the equation from Table 6-5 and parameters from Table 6-4. This value provides the maximum output voltage possible from the bridge under normal operating conditions and corresponds to the maximum load that can be applied to the bridge, Load(Bridge Max). If the system does not use the entire output range of the bridge, VOUT(System Max) defines the maximum differential output signal that is applied to a specific system and Load(System Max) is the corresponding maximum load. For example, if VOUT(Bridge Max) corresponds to Load(Bridge Max) = 5 kg, but the system specifications only require that Load(System Max) = 2.5 kg, then VOUT(System Max) is given by Equation 42:
Note that if Load(System Max) = Load(Bridge Max), then VOUT(System Max) = VOUT(Bridge Max).
After VOUT(System Max) has been determined, choose the corresponding gain value for the ADC PGA. The amplifier gain should be the largest allowable value that is still less than the ADC FSR. In some cases it is not possible to choose an amplifier gain that uses the entire ADC FSR. While this is often an acceptable tradeoff between resolution and ease-of-use, care should be taken to ensure that all system requirements are still met when the ADC FSR cannot be maximized.
Next, ensure that the bridge common-mode voltage, VCM(Bridge), defined in Table 6-5 is within the common-mode range of the ADC amplifier, VCM(ADC), under a no-load condition (R1 = R2 = R3 = R4). The amplifier common-mode range varies by component, and will be defined in the data sheet based on the gain setting and supply voltage. However, targeting VCM(Bridge) = AVDD / 2 is a good choice as this is typically in the center of the VCM(ADC) range, enabling the highest gain possible per the previous step. Moreover, the bridge configuration in Figure 6-2 inherently sets VCM(Bridge) to AVDD / 2 under a no-load condition when VEXCITATION = AVDD.
Finally, follow the instructions in Section 5.5 if calibration is required.