# Seemingly Simple Circuits, Part 1: The One-Op-Amp Diff-Amp

The following is Part 1 of a four-part series.

The basic one-op-amp differential amplifier consists of one op-amp and four resistors. Yet few have contemplated the depth of its complexity. It is studied in undergraduate engineering school and is familiar to analog-circuit engineers. Yet familiarity can easily be mistaken for understanding. Most of us have used it multiple times in designs. This article is intended take some readers deeper into diff-amp theory than they might have thought even existed, yet what is presented can reveal otherwise inexplicable design problems with this simple circuit.

A differential amplifier , or diff-amp for short, is a two-port circuit that inputs two quantities and amplifies their difference. The most familiar example is the op-amp, with inputs marked + and – and with a voltage gain that is ideally infinite. Op-amps can be used to construct finite-gain differential amplifiers or diff-amps for short. The most commonly used and simplest is the one-op-amp diff-amp , shown below, with input-range offset and common-mode (CM) voltage extension; the third voltage, VOS , has been included along with two offset resistors, ROS+ and ROS– . The differential input voltage of a diff-amp is defined as: The difference of two voltages as vI tells us nothing about their actual values, which can be far removed from 0 V while their difference can be within a specified input range. The common-mode (CM) voltage is defined as It is the voltage added to both of the differential inputs relative to input ground (0 V). The CM voltage is simply the average voltage of the two input terminals. The input voltages straddle vCM and from the above two equations are Both + and − inputs are floating above ground at the CM voltage. Set vI = 0 (shorted input terminals) so that vI+ = vI- and vCM is applied to both input terminals. It is simply the input offset of vI .

The output voltage of the amplifier can be expressed in either of the two input voltages, or as their differential and common-mode combinations: (Offset voltage VOS as a third input voltage is included later.) The CM voltage gain ACM and differential voltage gain Av can be expressed in the voltage gains of each input to the output as and

For an ideal differential amplifier, the gains of the two inputs are of the same magnitude and ACM = 0. These basic equations apply to diff-amps generally.

The amplifier gains can be expressed in circuit component values by solving the one-op-amp diff-amp circuit in various ways. Here, a path less traveled will illustrate a simplifying method based on finding the node resistances at the op-amp inputs. This can be accomplished by inspection, assuming the inputs are driven by voltage sources. Then where || is the parallel math operation. These node resistances can be used in divider formulas as follows: where Rout and Rin are the divider output and input resistances. Applying divider formulas and voltage superposition to the circuit, The op-amp output is where K is the op-amp open-loop differential gain. When K approaches infinity, then The usefulness of this rather involved form of the op-amp output equation that includes each resistance is that it allows us to later analyze the effects of resistance tolerance on accuracy. Ideally, Under these ideal conditions, and the input CM voltage range is where V+max is the maximum v+ voltage of the op-amp input range. For rail-to-rail-input (RRI) op-amps, this is the op-amp positive supply voltage.

Adding ROS+ and ROS– to the circuit do not change either of the above two formulas. The ROS increase the CM input voltage range by increasing the divider input attenuation (by making R+ smaller) and at the same time increase the op-amp feedback divider attenuation which increases the non-inverting closed-loop gain. The effects of the two dividers cancel so that Av is unaffected. However, there is an effect on the circuit in that by dividing down more from the input and then amplifying more, the output is noisier and the op-amp input offset voltage, VIOS , is also amplified more. The advantage is that the CM range is extended by the increased input attenuation but at the design cost of a more precise and less noisy op-amp.

This amplifier can be used before the ADC in data-acquisition systems to provide a wider range for the input voltage than the ADC allows. For instance, suppose a single-supply, 10-bit ADC is driven by it, and the ADC has an input range of 0 V to 5 V. It is desired that the differential input span a range of ±2.5 V with a common-mode range of 0 V to over 30 V. By adding the ROS resistors, a given differential gain, Av , can be chosen while extending the CM input voltage range. Otherwise, omitting the ROS resistors, Rf+ can be offset (as shown) by VOS with the same gain equation, but for a given Av , the CM range will also be determined. The above formula for vCM is valid, but Ri+ /R+ is determined by Rf+ and Ri+ .

The amplifier shown above has three inputs and one output and can be represented by a block diagram based on the above vO equation, as shown below. These are the equations in graphical form. ## 2 comments on “Seemingly Simple Circuits, Part 1: The One-Op-Amp Diff-Amp”

1. bjcoppa
September 30, 2014

It would be interesting to compare the top 3 producers of op-amps in terms of optimal performance. Microchip is one of the leading manufacturers for industrial market segments. It is highly commoditized but innovation still occurs on a regular basis to improve efficiency.

2. Davidled
October 6, 2014

Nonlinear equation might be involved in the Op Amp with some parameters including current limit, slew rate and output clamp to analyze the magnitude and phase according to frequency input: low frequency range and high frequency range.

I am wondering what type of Op Amp actually represents the symbol of Op Amp shown in figures, because a different device might have its own unique character of frequency response and transient response.

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