An amplifier is an analogue circuit. This page is about a voltage amplifier based on an Op-Amp. The output voltage (V_{out}) of the circuit depends on the input voltage (V_{in}) and the Gain (A_{v}) of the circuit.

It is a good idea to read the amplifier basics page first.

For all the circuits shown below, the amplifier is assumed to a have a positive and a negative power supply, usually ±15V, so that the output voltage can be both positive and negative.

The Op-Amp needs to have ± power supplies (assumed to be ±15V)

The non-inverting input is connected to 0V

The circuit uses a feedback resistor (R_{f}) and an input resistor (R_{i})

Voltage gain (A_{v}) is determined by R_{i} and R_{f}

The voltage gain is given by:

A_{v} = −R_{f} / R_{i}

Note: R

The output voltage is directly proportional to the input voltage (as long as the output is not saturated) such that:

V_{out} = A_{v} × V_{in}

Note: If A

If the input voltage is positive, the output voltage is negative

If the input voltage is negative, the output voltage is positive

The graph shows the transfer characteristics (Input Voltage and Output Voltage) for an Inverting amplifier with a voltage Gain of −2

When V_{in} = +5V then V_{out} = −10V and when V_{in} = −5V then V_{out} = +10V

The Output Voltage is limited to ±13V by the power supply of the amplifier. Therefore, when V_{in} > +6.5V then V_{out} saturates at −13V and when V_{in} < −6.5V then V_{out} saturates at +13V (shown by the horizontal lines on the graph)

The graph shows the relationship between the Input Voltage and Output Voltage of an Inverting amplifier with a voltage Gain of −2 when the input is an A.C. voltage

At all times V_{out} = −2 × V_{in}

The voltage gain is:

A_{v} = − 220 ×10^{3} / 100 ×10^{3} = −2.2

If V_{in} = +1.0V then V_{out} = −2.2V

The Input Voltage has been amplified (made bigger)

The voltage gain is:

A_{v} = − 47 ×10^{3} / 100 ×10^{3} = −0.47

If V_{in} = +1.0V then V_{out} = −0.47V

The Input Voltage has been attenuated (made smaller)

The voltage gain is:

A_{v} = − 100 ×10^{3} / 100 ×10^{3} = −1.0

If V_{in} = +1.0V then V_{out} = −1.0V

This is a unit gain amplifier - the Output Voltage has the same amplitude as the Input Voltage. This amplifier is a buffer as the input takes almost no current from the voltage source but provides a reasonable current to the subsequent circuits

The voltage gain is:

A_{v} = − 100 / 100 = −1.0

This is a poor circuit as the resistor values are too small. The amplifier will draw too much current from the source. Resistor values should always be greater than 1kΩ

The two main parameters of the Inverting Amplifier are the gain and the bandwidth. Increasing the gain reduces the bandwidth and vice versa.

For an inverting amplifier based on a standard Op-Amp the relationship between gain and bandwidth is approximately:

gain × bandwidth = 10^{6}

The graph shows that as gain increases, bandwidth decreases. Note that both scales are logarithmic. The Gain axes shows the magnitude of the gain and the negative sign is ignored

When the gain is ×1 (blue line) the amplifier works effectively up to frequencies of 1MHz. If the gain is increased to ×10 (green line)the amplifier only works effectively up to about 100kHz (still okay for audio) but at a gain of ×1000 (red line)the amplifier only works effectively up to a frequency of 1KHz before the gains starts to reduce and the Output Voltage starts to decrease

If the gain is −100, the bandwidth is 10kHz

If a bandwidth of 40kHz is required, the maximum gain is −25

When used in reality, amplifiers are often decoupled which means that the input and output are connected through capacitors to stop any spurious D.C. signals compromising the performance of the amplifier. Depending on what the amplifier is attached to, a resistor may also be needed on the output down to 0V.

The capacitor on the input is usually a non-electrolytic type, nominally 1µF or less. The capacitor on the output is ideally a non-electrolytic type but sometimes larger value electrolytic capacitors need to used if the amplifier is providing significant current to the next stage

The addition of capacitors to the input and output can reduce the bandwidth of the amplifier

When considering amplifiers made from Op-Amps there are two basic assumptions:

- The open loop gain (A
_{0}) of the Op-Amp is very large - No current flows in to the inverting and non-inverting inputs

**Negative Feedback**

- Recall that V
_{out}= A_{0}× (V_{+}− V_{−}) where A_{0}= 10^{6}and so a difference between V_{+}and V_{−}of more than a few µV will result in a large (saturated) output voltage - The feedback resistor ensures that voltage at the inverting input is very similar (within a few microvolts) to the voltage at the non-inverting input
- As the non-inverting input is connected to ground (0V) then the inverting input must also be very close to 0V and is called a virtual earth
- R
_{i}and R_{f}form a potential divider with V_{in}at one end, V_{out}at the other end and the inverting input at approximately 0V in the middle - The feedback works because if V
_{in}is positive and rises, the voltage at the inverting input rises as a consequence. This increases the difference between the inverting and non-inverting inputs and causes V_{out}to change. As the inverting input is bigger than the non-inverting input in this case then V_{out}becomes more negative. As V_{out}becomes more negative the voltage at the inverting input falls again until it is approximately 0V once more. Therefore a change in the input voltage causes an opposing change in the output voltage to keep the inverting input at (or very close to) zero

**Gain Equation**

- Assume V
_{in}is positive (as shown in the diagram above) - The current in the input resistor is given by I = V
_{in}/ R_{i}because the virtual earth means that the V_{in}is the potential difference across the resistor - As no current flows in to the inverting input, the current in the input resistor also flows through the feedback resistor
- To make the current flow from the virtual earth in the direction shown V
_{out}must be negative - Therefore I = −V
_{out}/ R_{f} - Equating the currents leads to the gain equation
- Recall, gain is defined as: Gain = V
_{out}/ V_{in}

We have

I = V_{in} / R_{i} = −V_{out} / R_{f}

and therefore

Gain = V_{out} / V_{in} = −R_{f} / R_{i}

© Paul Nicholls

October 2018

Electronics Resources by Paul Nicholls is licensed under a Creative Commons Attribution 4.0 International License.