SBOA590 November   2024 OPA186 , OPA206 , OPA328 , OPA391 , OPA928

 

  1.   1
  2.   Abstract
  3.   Trademarks
  4. 1Input Offset Voltage (VOS) Definition
    1. 1.1 Input Offset Voltage Drift (dVOS/dT) Definition
    2. 1.2 VOS and VOS Temperature Drift Inside the Amplifier
    3. 1.3 Laser Trim to Adjust Performance
    4. 1.4 Package Trim (e-Trim™) to Adjust Performance
  5. 2Input bias current (IB) definition
    1. 2.1 Input Bias Current (IB) and IB Temperature Drift Inside the Amplifier
    2. 2.2 Derivation of IB Conversion to VOS
    3. 2.3 Internal Bias Current Cancelation
    4. 2.4 Super Beta Input Transistors
  6. 3Other Factors Influencing Offset
    1. 3.1 Finite Open Loop Gain (AOL)
    2. 3.2 Common Mode Rejection Ratio (CMRR)
    3. 3.3 Power Supply Rejection Ratio (PSRR)
    4. 3.4 AOL, CMRR, and PSRR Over Frequency
    5. 3.5 Electromagnetic Interference Ratio (EMIRR)
    6. 3.6 Mechanical Stress Induced Offset Shift
    7. 3.7 Parasitic Thermocouples
    8. 3.8 Flux Residue and Cleanliness
  7. 4Zero-drift Amplifiers to Minimize VOS and VOS Drift
  8. 5Calibration of VOS, IB, and Gain Error
  9. 6References
  10. 7Revision History

Finite Open Loop Gain (AOL)

The open-loop-gain (AOL) for an op amp is defined as the change in output over the change in the differential input of the op amp. For an ideal op amp the differential input is considered to be zero and the AOL is infinite. For a practical op amp, however, the differential input is the input offset voltage (VOS) and the open loop gain is typically on the order of 1 MV/V or 120 dB. The equation for AOL is AOL = ΔVOUT/ ΔVOS or 20log(ΔVOUT/ ΔVOS) in decibels. Rearranging the equation shows that VOS changes when the output signal changes by ΔVOS = ΔVOUT/AOL. Figure 3-1 shows an inverting amplifier in a gain of –1 V/V where the output swings from -12 V to +12 V. Because the inverting configuration is used the common mode voltage (VCM) is held constant at 0 V. Changing common mode also causes a shift in offset, so the inverting configuration is useful in illustrating the effect of AOL on offset without compounding the effect with Vcm.

The specifications for the OPA210 example are shown in Table 3-1. Based on the specification, you would expect the typical offset to be ±5 µV. Notice the test condition listed at the top of the table indicates that the parameters all assume VCM = VOUT = midsupply. However, the output voltage ranges from -12 V to +12 V, and the common mode is at 0 V. Thus, the 24 V change in output voltage will result in a corresponding 6 µV change in offset (see calculation Equation 30, and simulation Figure 3-2). In the simulation notice that VOS = 5 µV specification when VOUT = 0 V as expected based on the test condition.

Equation 29. AOL(lin)=10AOL(dB)/20=10132dB/20=3.981106 V/V
Equation 30. ΔVOS=ΔVOUTAOL(lin)=24 V3.981106 V/V=6.0 μV
OPA206 VOS Shift Due to
                    Finite AOL on Inverting OPA210 Configuration Figure 3-1 VOS Shift Due to Finite AOL on Inverting OPA210 Configuration
OPA206 Simulated VOS and
                    Output Swing for Inverting OPA210 Circuit Figure 3-2 Simulated VOS and Output Swing for Inverting OPA210 Circuit