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Chapter 8: OPERATIONAL AMPLIFIERS

# Averager and Summer Circuits

If we take three equal resistors and connect one end of each to a common
point, then apply three input voltages (one to each of the resistors'
free ends), the voltage seen at the common point will be the
mathematical *average* of the three.

This circuit is really nothing more than a practical application of Millman's Theorem:

This circuit is commonly known as a *passive averager*, because it generates an average voltage with non-amplifying components. *Passive*
simply means that it is an unamplified circuit. The large equation to
the right of the averager circuit comes from Millman's Theorem, which
describes the voltage produced by multiple voltage sources connected
together through individual resistances. Since the three resistors in
the averager circuit are equal to each other, we can simplify Millman's
formula by writing R_{1}, R_{2}, and R_{3} simply as R (one, equal resistance instead of three individual resistances):

If we take a passive averager and use it to connect three input voltages
into an op-amp amplifier circuit with a gain of 3, we can turn this *averaging* function into an *addition* function. The result is called a *noninverting summer* circuit:

With a voltage divider composed of a 2 kΩ / 1 kΩ combination, the
noninverting amplifier circuit will have a voltage gain of 3. By taking
the voltage from the passive averager, which is the sum of V_{1}, V_{2}, and V_{3} divided by 3, and multiplying that average by 3, we arrive at an output voltage equal to the *sum* of V_{1}, V_{2}, and V_{3}:

Much the same can be done with an inverting op-amp amplifier, using a
passive averager as part of the voltage divider feedback circuit. The
result is called an *inverting summer* circuit:

Now, with the right-hand sides of the three averaging resistors
connected to the virtual ground point of the op-amp's inverting input,
Millman's Theorem no longer directly applies as it did before. The
voltage at the virtual ground is now held at 0 volts by the op-amp's
negative feedback, whereas before it was free to float to the average
value of V_{1}, V_{2}, and V_{3}. However, with
all resistor values equal to each other, the currents through each of
the three resistors will be proportional to their respective input
voltages. Since those three currents will *add* at the virtual ground node, the algebraic sum of those currents through the feedback resistor will produce a voltage at V_{out} equal to V_{1} + V_{2} + V_{3}, except with reversed polarity. The reversal in polarity is what makes this circuit an *inverting* summer:

Summer (adder) circuits are quite useful in analog computer design, just as multiplier and divider circuits would be. Again, it is the extremely high differential gain of the op-amp which allows us to build these useful circuits with a bare minimum of components.

**REVIEW:**- A
*summer*circuit is one that*sums*, or adds, multiple analog voltage signals together. There are two basic varieties of op-amp summer circuits: noninverting and inverting.

## Related Content:

Circuits: Noninverting summer.

Circuits: Inverting summer.