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

 

  1.   1
  2.   Abstract
  3.   Trademarks
  4. 1Bridge Overview
  5. 2Bridge Construction
    1. 2.1 Active Elements in Bridge Topologies
      1. 2.1.1 Bridge With One Active Element
        1. 2.1.1.1 Reducing Non-Linearity in a Bridge With One Active Element Using Current Excitation
      2. 2.1.2 Bridge With Two Active Elements in Opposite Branches
        1. 2.1.2.1 Eliminating Non-Linearity in a Bridge With Two Active Elements in Opposite Branches Using Current Excitation
      3. 2.1.3 Bridge With Two Active Elements in the Same Branch
      4. 2.1.4 Bridge With Four Active Elements
    2. 2.2 Strain Gauge and Bridge Construction
  6. 3Bridge Connections
    1. 3.1 Ratiometric Measurements
    2. 3.2 Four-Wire Bridge
    3. 3.3 Six-Wire Bridge
  7. 4Electrical Characteristics of Bridge Measurements
    1. 4.1 Bridge Sensitivity
    2. 4.2 Bridge Resistance
    3. 4.3 Output Common-Mode Voltage
    4. 4.4 Offset Voltage
    5. 4.5 Full-Scale Error
    6. 4.6 Non-Linearity Error and Hysteresis
    7. 4.7 Drift
    8. 4.8 Creep and Creep Recovery
  8. 5Signal Chain Design Considerations
    1. 5.1 Amplification
      1. 5.1.1 Instrumentation Amplifier
        1. 5.1.1.1 INA Architecture and Operation
        2. 5.1.1.2 INA Error Sources
      2. 5.1.2 Integrated PGA
        1. 5.1.2.1 Integrated PGA Architecture and Operation
        2. 5.1.2.2 Benefits of Using an Integrated PGA
    2. 5.2 Noise
      1. 5.2.1 Noise in an ADC Data Sheet
      2. 5.2.2 Calculating NFC for a Bridge Measurement System
    3. 5.3 Channel Scan Time and Signal Bandwidth
      1. 5.3.1 Noise Performance
      2. 5.3.2 ADC Conversion Latency
      3. 5.3.3 Digital Filter Frequency Response
    4. 5.4 AC Excitation
    5. 5.5 Calibration
      1. 5.5.1 Offset Calibration
      2. 5.5.2 Gain Calibration
      3. 5.5.3 Calibration Example
  9. 6Bridge Measurement Circuits
    1. 6.1 Four-Wire Resistive Bridge Measurement with a Ratiometric Reference and a Unipolar, Low-Voltage (≤5 V) Excitation Source
      1. 6.1.1 Schematic
      2. 6.1.2 Pros and Cons
      3. 6.1.3 Parameters and Variables
      4. 6.1.4 Design Notes
      5. 6.1.5 Measurement Conversion
      6. 6.1.6 Generic Register Settings
    2. 6.2 Six-Wire Resistive Bridge Measurement With a Ratiometric Reference and a Unipolar, Low-Voltage (≤ 5 V) Excitation Source
      1. 6.2.1 Schematic
      2. 6.2.2 Pros and Cons
      3. 6.2.3 Parameters and Variables
      4. 6.2.4 Design Notes
      5. 6.2.5 Measurement Conversion
      6. 6.2.6 Generic Register Settings
    3. 6.3 Four-Wire Resistive Bridge Measurement With a Pseudo-Ratiometric Reference and a Unipolar, High-Voltage (> 5 V) Excitation Source
      1. 6.3.1 Schematic
      2. 6.3.2 Pros and Cons
      3. 6.3.3 Parameters and Variables
      4. 6.3.4 Design Notes
      5. 6.3.5 Measurement Conversion
      6. 6.3.6 Generic Register Settings
    4. 6.4 Four-Wire Resistive Bridge Measurement with a Pseudo-Ratiometric Reference and Asymmetric, High-Voltage (> 5 V) Excitation Source
      1. 6.4.1 Schematic
      2. 6.4.2 Pros and Cons
      3. 6.4.3 Parameters and Variables
      4. 6.4.4 Design Notes
      5. 6.4.5 Measurement Conversion
      6. 6.4.6 Generic Register Settings
    5. 6.5 Four-Wire Resistive Bridge Measurement With a Ratiometric Reference and Current Excitation
      1. 6.5.1 Schematic
      2. 6.5.2 Pros and Cons
      3. 6.5.3 Parameters and Variables
      4. 6.5.4 Design Notes
      5. 6.5.5 Measurement Conversion
      6. 6.5.6 Generic Register Settings
    6. 6.6 Measuring Multiple Four-Wire Resistive Bridges in Series with a Pseudo-Ratiometric Reference and a Unipolar, Low-Voltage (≤5V) Excitation Source
      1. 6.6.1 Schematic
      2. 6.6.2 Pros and Cons
      3. 6.6.3 Parameters and Variables
      4. 6.6.4 Design Notes
      5. 6.6.5 Measurement Conversion
      6. 6.6.6 Generic Register Settings
    7. 6.7 Measuring Multiple Four-Wire Resistive Bridges in Parallel Using a Single-Channel ADC With a Ratiometric Reference and a Unipolar, Low-Voltage (≤ 5 V) Excitation Source
      1. 6.7.1 Schematic
      2. 6.7.2 Pros and Cons
      3. 6.7.3 Parameters and Variables
      4. 6.7.4 Design Notes
      5. 6.7.5 Measurement Conversion
      6. 6.7.6 Generic Register Settings
    8. 6.8 Measuring Multiple Four-Wire Resistive Bridges in Parallel Using a Multichannel ADC With a Ratiometric Reference and a Unipolar, Low-Voltage (≤ 5 V) Excitation Source
      1. 6.8.1 Schematic
      2. 6.8.2 Pros and Cons
      3. 6.8.3 Parameters and Variables
      4. 6.8.4 Design Notes
      5. 6.8.5 Measurement Conversion
      6. 6.8.6 Generic Register Settings
  10. 7Summary
  11. 8Revision History

Design Notes

In the asymmetric, high-voltage supply configuration, the excitation voltage applied to the bridge, VEXCITATION, cannot typically be used as the ADC supply voltage. Instead, an additional lower-voltage supply (≤ 5 V) is required to power the ADC. Moreover, the ADC cannot directly use the high-voltage excitation source as the differential reference voltage, VREF, and instead requires an attenuation circuit. Typically, a simple resistor divider is used as shown in Figure 6-5, though other options include a difference amplifier or a discrete voltage reference. Using a resistor divider or an amplifier can introduce errors between the bridge and the reference inputs that are not present between the bridge and the ADC inputs, resulting in a pseudo-ratiometric reference configuration. Choosing a discrete voltage reference results in a non-ratiometric configuration. Finally, choose the asymmetric supply voltages such that the bridge output common-mode voltage is within the lower-voltage input range of the ADC. Otherwise, additional input signal conditioning circuitry is necessary.

A four-wire resistive bridge measurement with a pseudo-ratiometric reference and asymmetric, high-voltage (> 5 V) supplies requires:

  • Differential analog inputs (AINP and AINN)
  • Differential reference inputs (REFP and REFN) or integrated voltage reference
  • Low-noise amplifier
  • High-voltage, asymmetric supplies
  • VREF attenuation circuit (resistor divider, difference amplifier, and so forth) or separate voltage reference

First, identify the maximum differential output voltage of the bridge, VOUT(Bridge Max), using the equation from Table 6-9 and parameters from Table 6-8. 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 52:

Equation 52. VOUT(System Max) = VOUT(Bridge Max) • (2.5 kg / 5 kg) = VOUT(Bridge Max) / 2

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 amplifier. The amplifier gain should be the largest allowable value that is still less than the ADC full-scale range (FSR). In some cases it is not possible to choose an amplifier gain that uses the entire ADC FSR, especially when an ADC with an integrated PGA is selected. While this is often an acceptable tradeoff between resolution and ease-of-use, ensure that all system requirements are still met when the ADC FSR cannot be maximized.

Next, choose the values of the asymmetric supplies such that the bridge common-mode voltage, VCM(Bridge), is within the common-mode range of the ADC amplifier under a no-load condition (R1 = R2 = R3 = R4). Typically, the target ADC amplifier common-mode voltage, VCM(ADC), is selected to be at the ADC mid-supply voltage (AVDD / 2), though this is not a requirement. The amplifier common-mode range varies by component, and is defined in the data sheet based on the gain setting and supply voltage.

Using VCM(ADC) and the selected bridge excitation voltage, VEXCITATION, the asymmetric excitation voltages VEXCITATION+ and VEXCITATION- can be determined using Equation 53 and Equation 54:

Equation 53. VEXCITATION+ = VCM(ADC) + (VEXCITATION / 2)
Equation 54. VEXCITATION- = VCM(ADC) – (VEXCITATION / 2)

After calculating VEXCITATION+ and VEXCITATION-, choose the system reference source. When selecting a discrete voltage reference, ensure this component is high accuracy and low-drift for best performance. To maintain a pseudo-ratiometric relationship between VEXCITATION and VREF, choose a resistor divider or a difference amplifier to attenuate the bridge excitation voltage. The resistor-divider method is more commonly-used and is shown in Figure 6-5 as three resistors in series. The reference voltage, VREF, is established across the center component, RREF. Equation 55 and Equation 56 determine the ratio of RTOP and RBOTTOM to RREF using VREF, the previously-determined VEXCITATION± values, and the voltage seen at the REFN pin (VREFN) in Figure 6-5:

Equation 55. RRATIO (TOP / REF) = [(VEXCITATION+ – VREFN) / VREF] – 1
Equation 56. RRATIO (BOTTOM / REF) = (VREFN – VEXCITATION-) / VREF

For example, consider a system with the following constraints:

  • VEXCITATION = 15 V
  • VCM(ADC) = VREF = 2.5 V
  • RREF = 4.7 kΩ
  • VREFN = 1.25 V

Use Equation 53 through Equation 56 to calculate the remaining system parameters:

  • VEXCITATION+ = 10 V
  • VEXCITATION- = –5 V
  • RRATIO (TOP / REF) = 2.5
  • RRATIO (BOTTOM / REF) = 2.5

Therefore, RTOP = RBOTTOM = 11.8 kΩ for this specific system. Figure 6-6 shows the various voltages (in blue) and resistor values (in red) that are used in this example.

GUID-20211110-SS0I-QKQS-FP4P-JWBCH27KJ9TH-low.svgFigure 6-6 Example Resistor and Voltage Values

Note that there are some implied constraints in Equation 55 and Equation 56, including VEXCITATION+ > VREFN > VEXCITATION-, VEXCITATION+ > VEXCITATION-, and VEXCITATION > VREF. Otherwise, nonsensical results may occur, such as negative resistance values. Ultimately, check that the results of each equation meet all of the final design requirements as well as make physical sense.

It is also important to allow headroom near the maximum absolute and differential reference voltages applied to the ADC. Many systems seek to maximize the ADC dynamic range by maximizing VREF. However, variations in the excitation voltage and resistor impedance may increase VREF beyond the operating range of the ADC, which is typically limited to AVSS on VREFN and AVDD on VREFP. Under these conditions, consider a small reduction in the RREF impedance to allow for system tolerances.

Select high accuracy (≤ 0.1%), low temperature-drift (≤ 10 ppm/°C) resistors for the reference path. Keep the nominal resistance value low to limit thermal noise. As an example, a 1-kΩ resistor at 25°C and 1-kHz bandwidth contributes 128 nVRMS of noise. These conditions are important to keep VREF as close as possible to being ratiometric with VEXCITATION and minimize overall measurement error. Additionally, buffers might be required depending on the impedance of the differential reference inputs of the ADC. The buffer can also introduce errors and further reduce the ratiometric relationship between VIN and VREF.

Finally, follow the instructions in Section 5.5 if calibration is required.