SBAS535D August 2013 – June 2026 ADS1120
PRODUCTION DATA
To stay within the linear operating range of the PGA, the input signals must meet certain requirements that are discussed in this section.
The outputs of both amplifiers (A1 and A2) in Figure 8-2 cannot swing closer to the supplies (AVSS and AVDD) than 200mV. If the outputs OUTP and OUTN are driven to within 200mV of the supply rails, the amplifiers saturate and consequently become nonlinear. To prevent this nonlinear operating condition the output voltages must meet Equation 6:
Translating the requirements of Equation 6 into requirements referred to the PGA inputs (AINP and AINN) is beneficial because there is no direct access to the outputs of the PGA. The PGA employs a symmetrical design, therefore the common-mode voltage at the output of the PGA can be assumed to be the same as the common-mode voltage of the input signal, as shown in Figure 8-3.
Figure 8-3 PGA
Common-Mode VoltageThe common-mode voltage is calculated using Equation 7:
The voltages at the PGA inputs (AINP and AINN) can be expressed as Equation 8 and Equation 9:
The output voltages (VOUTP and VOUTN) can then be calculated as Equation 10 and Equation 11:
The requirements for the output voltages of amplifiers A1 and A2 (Equation 6) can now be translated into requirements for the input common-mode voltage range using Equation 10 and Equation 11, which are given in Equation 12 and Equation 13:
To calculate the minimum and maximum common-mode voltage limits, the maximum differential input voltage (VINMAX) that occurs in the application must be used. VINMAX can be less than the maximum possible FS value.
In addition to Equation 12, the minimum VCM must also meet Equation 14 because of the specific design implementation of the PGA.
Figure 8-4 and Figure 8-5 show a graphical representation of the common-mode voltage limits for AVDD = 3.3V and AVSS = 0V, with gain = 1 and gain = 16, respectively.

| AVDD = 3.3V |

| AVDD = 3.3V |
The following
discussion explains how to apply Equation 12 through Equation 14 to a hypothetical application. The setup for this example is AVDD =
3.3V,
AVSS =
0V, and
gain = 16, using an external reference,
VREF
= 2.5V.
The maximum possible differential input voltage VIN =
(VAINP
–
VAINN)
that can be applied is then limited to the full-scale range of FSR =
±2.5V /
16 =
±0.156V.
Consequently, Equation 12 through Equation 14 yield an allowed VCM range of
1.45V ≤
VCM ≤
1.85V.
If the sensor signal connected to the inputs in this hypothetical application does not make use of the entire full-scale range but is limited to VINMAX = ±0.1V, for example, then this reduced input signal amplitude relaxes the VCM restriction to 1.0V ≤ VCM ≤ 2.3V.
In the case of a fully-differential sensor signal, each input (AINP, AINN) can swing up to ±50mV around the common-mode voltage (VAINP + VAINN) / 2, which must remain between the limits of 1.0V and 2.3V. The output of a symmetrical Wheatstone bridge is an example of a fully-differential signal. Figure 8-6 shows a situation where the common-mode voltage of the input signal is at the lowest limit. VOUTN is exactly at 0.2V in this case. Any further decrease in common-mode voltage (VCM) or increase in differential input voltage (VIN) drives VOUTN below 0.2V and saturates amplifier A2.
Figure 8-6 Example
Where
VCM is at Lowest LimitIn contrast, the signal of an RTD is
of a pseudo-differential nature (if implemented as shown in the RTD Measurement section), where the negative input is held at a
constant voltage other than
0V and
only the voltage on the positive input changes. When a pseudo-differential signal
must be measured, the negative input in this example must be biased at a voltage
between
0.95V
and
2.25V.
The positive input can then swing up to
VINMAX
= 100mV
above the negative input.
In
this case the common-mode voltage changes at the same time the voltage on the
positive input changes. That is, while the input signal swings between
0V ≤
VIN ≤
VINMAX,
the common-mode voltage swings between
VAINN
≤ VCM ≤
VAINN
+ ½
VINMAX.
.The
requirements for the entire signal range are met if the common-mode voltage
requirements for the maximum input voltage VINMAX are
satisfied.
Figure 8-7 and Figure 8-8 show examples of both fully-differential and pseudo-differential signals, respectively.


Remember, common-mode voltage requirements with PGA enabled (Equation 12 to Equation 14) are as follows: