AN103: Common Mode Voltage

The assumptions made in developing Equations 1 and 2 are not always completely possible; however, they provide the reader with an insight into the parameters responsible for establishing "gains". Equations 1 and 2 are single ended (SE) output expressions with two terms;

1. a gain term multiplying the differential input, and
2. another gain term multiplying the SE input voltage.
Note: This common SE term is the origin of common mode voltage gain.

Instrumentation amplifiers typically have several internal differential pairs, all of which contribute to developing the final SE output, which includes a net common mode gain term. Designers and manufacturers of IC instrumentation amplifiers use two techniques to diminish this common mode term;

1. ensure internal differential pairs have matched devices, and
2. use topologies that use large dynamic values of Rss.

Note: The SE term is diminished as Rss increases provided the stated conditions of "identity" are true. Therefore, differential input IC amplifiers have very large dynamic values of Rss and differential pair cells with near identical devices. Unfortunately, such ideal conditions can not be completely achieved. Consequently, there will always be some common mode gain ( Acm). An exact numerical solution for the output voltages Vo1, Vo2 in the topology shown in Figure 3 illustrates the validity of our assumptions. Table 1 illustrates matrix solutions for two different cases using the device parameters shown in Figure 3.

Case 1: Identical devices with 10 volts of common mode voltage, two different Rss values of 5 MegΩ and 50 MegΩ show that;

1. SE outputs do have a common mode gain, which decreases as Rss increases.
2. There is no DE output, (no common mode gain).

Case 2: Non-identical devices with 10 volts of common mode voltage, two different Rss values of 5 MegΩ and 50 MegΩ, combined with random 1% tolerance on device parameters show that;

1. SE outputs do have a common mode gain that decreases as Rss increases.
2. There are DE outputs; consequently, a common mode DE output gain exists.

It is clear that in the practical real world, semiconductor amplifiers inherently have a common mode gain. The instrumentation engineer should be aware of this fact and use quality instrumentation modules and avoid application topologies with large common mode voltages.

Practical Examples of Common Mode Voltages

Figure 4 illustrates a typical field sensor that generates a net differential signal and includes both the sensor common mode voltage source (Vcm, Rscm) and a common mode voltage source (Vx, Rx) contribution from the difference between the field ground and data acquisition system ground.


The wiring between a field sensor and its associated signal-conditioning module is subject electro-magnetic induced voltages. These induced voltages can add both an additional common mode voltage source and a differential input error voltage. Analysis of this phenomenon is beyond the scope of this document. Figure 5 illustrates two different topologies for measuring load currents using shunt resistors.


Case A is a differential voltage (V1a/V2a) measurement across a shunt inserted in the supply line. In this case, the common mode voltage is equivalent to the supply voltage plus the voltage difference between the field ground and DAS ground.

Case B is, again, a differential voltage (V1b/field-ground) measurement across a shunt inserted in the field ground line. A differential measurement is recommended here to eliminate the error caused by the common mode voltage equivalent to the voltage difference between the field ground and DAS ground. Figure 6 illustrates a standard bridge sensor, which is often the basis for industrial measurements.