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What is an Operational Amplifier?

Operational amplifiers, (op-amp), are linear devices that are used extensively in signal conditioning, filtering, or to perform mathematical operations such as adding, subtracting, integration, and differentiation.

They are used in combination with external feedback components such as resistors, capacitors and inductors between the input and output. The configuration of these components determines the function/operation of the op-amp.

They have a three-terminal device with two high impedance inputs. The input designated by a minus sign, (-), is called the "inverting" input, while the other input is designated by a plus sign, (+) us , is called the "non-inverting" input. The third terminal represents the op-amps output which can sink or source either a voltage or current. The output signal is the amplification factor or amplification gain (A) and is multiplied by the input signal. Depending on the nature of the input or output, there are four classifications for op-amp gain [2].

Equivalent Circuit

Op-Amp Parameter and Idealized Characteristic

The op-amp output is limited by the +V_supply and the -V_supply where they are the upper and lower limit of the op-amp respectively [2].

Inverting Op-Amp

The main feature of this circuit is the gain that it produces which can be calculated as: [3]

This configuration has applications in audio mixers and provides low impedance. Another application is that since the output it generates is phase shifted 180 degrees, it can be used as a phase shifter [4].

 Non-Inverting Op-Amp

The gain of the circuit can be calculated as:

This configuration is one of the most popular and widely used forms of op-amp circuits. It is primarily used in applications where high input impedance is required [3].

Summing Amplifier

The summing amplifier also known as a linear mixer sums all the signals in a completely linear fashion. The other type of mixer is called a multiplying mixer and uses the non-linear properties of circuits to multiply two signals together and generate additional frequencies.

The output of the circuit can be calculated as:

Where R1x is the value of the resistor at the input. This configuration provides the ideal platform for audio mixing. The various inputs (R1a, R1b, R1c etc.) can be controlled independently as the virtual earth (a node of the circuit maintained at a steady reference potential without being directly connected [5]) of the inverting amplifier is not dependent on the conditions of any of the inputs [3].

Differential Amplifier

The

ideal voltage output of a differential amplifier is:

If all resistors are equal, that is: R1=R2=R3=R4, then the circuit will become a Unity Gain Differential Amplifier and V_out is simply:

The differential amplifier configuration can be used by adding more resistors in parallel with the input resistors to make it either add or subtract voltages applied to the respective inputs. A common method of doing this is to connect a "Resistive Bridge" (Wheatstone Bridge) to the input of the an op-amp [3].

Integrator Amplifier

In this configuration, by changing the resistive feedback element to a capacitor, we create an RC network across the op-amps feedback path creating an Op-Amp Integrator circuit. This circuit performs integration as the output responds to changes in the input voltage over time since the op-amp produces an output voltage that is proportional to the integral of the input voltage.

The ideal voltage output of an integrator amplifier is:

This can be re-written as:

Where ω = 2πƒ and V_out is a constant 1/RC times the integral of the input voltage V_IN with respect to time and is phase shifted 180° as indicated by the negative [4].

The integrator amplifier circuit has many applications. They are most commonly seen in analog-to-digital converters, ramp generators, and in wave shaping. They also see usage in analog computers to perform calculus operations [6].

Differentiator Amplifier

In this configuration compared to the integrator amplifier, the resistor and capacitor have reversed positions and now reactance is connected to the input. This circuit performs differentiation as the voltage output it produces is directly proportional to the input voltage's rate-of-change with respect to time.

The ideal voltage of the differentiator amplifier is:

Thus the output voltage is a constant, -R_f*C times the derivative of the input voltage with a 180° phase shift as indicated by the negative [3].

The differentiator amplifier circuit are most commonly designed to operate on triangular and rectangular signals. They also see usage as wave shaping circuits to detect high frequency components in the input signal [7].

Schmitt Trigger

A Schmitt trigger is a comparator circuit (, a circuit that compares two voltages and outputs either a 1 or 0 depending on which is larger) , that implements hysteresis (, the dependence of the state of a system on its history) , by applying positive feedback to the non-inverting input of the op-amp. In the non-inverting configuration, when V_in is greater than some chosen threshold as indicated by V_ref , then the output is high, or V_SAT . If the input becomes less than V_ref , the output will become V_-SAT . This dual threshold is called hysteresis and allows the Schmitt trigger to be used as a bistable multivibrator multi-vibrator (latch or flip-flop). They are very similar to the basic inverting and non-inverting op-amp configurations except that the inputs are switched.

Schmitt triggers are usually used in signal conditioning applications to remove noise from signals in digital circuits, particularly in mechanical contact bounce in switches. Other applications include closed loop negative feedback, relaxation oscillators, function generators and switching power supplies [8].

Contributors:

Faculty Advisors: Kim Pope, John Thistle, Allyson Giannikouris, Michael Lenover (alumni)