Why are voltage followers prone to oscillation?

Operational amplifier (op-amp) amplification circuits commonly utilize negative feedback. However, op-amps have a pole (transition point) that can cause phase lag within the bandwidth, resulting in positive feedback. On the other hand, voltage followers (unity gain amplifiers) employ full feedback, and their bandwidth extends up to the cutoff frequency, making them prone to oscillation. When using voltage followers, it is essential to select products that operate at unity gain.

Fig. 1 Oscillation due to feedback
Fig. 1 Oscillation due to feedback

In amplification circuits using operational amplifiers (op-amps), feedback loops are commonly employed. However, under certain conditions, these feedback loops can lead to oscillation. This phenomenon is known as the oscillation condition and is characterized by gain and phase criteria. To put it simply, oscillation occurs when the input signal or noise, as shown in the diagram, is gradually amplified through feedback (see Fig. 1).
Mathematically, this can be expressed as follows:
           β x A ≧ 1
           ∠ β x A         ≧ 360°
In other words, oscillation occurs when a signal greater than the original input is fed back and added in phase.

Let’s illustrate the frequency characteristics of a standalone operational amplifier (op-amp) using a graph.
Gain Curve and Poles:

  • The gain curve of an op-amp exhibits poles (transition points).
  • From the first pole frequency, the gain decreases with a slope of -20 dB/decade.
  • If there are two poles, the second pole frequency results in a steeper slope of -40 dB/decade.
  • Additionally, the phase shift at this pole frequency is delayed by 90° for a single pole.
  • With two poles, the total phase shift amounts to 180°.

Unity Gain and Phase Shift:

  • In commonly used op-amps not designed for unity gain operation, there are two gain poles within the bandwidth up to the cutoff frequency (zero-crossing frequency) (f_T).
  • However, op-amps specifically designed for unity gain operation typically have only one pole within the bandwidth.
  • Consequently, the phase shift is limited to 90°.

These characteristics are essential for understanding op-amp behavior, especially when designing feedback circuits. The unity gain frequency and phase shift play crucial roles in determining the usable frequency range of an op-amp circuit.

Fig. 2 Frequency characteristics of operational amplifiers that cannot be used with unity gain
Fig. 2 Frequency characteristics of operational amplifiers that cannot be used with unity gain
Fig. 3 Frequency characteristics of operational amplifiers that can be used with unity gain
Fig. 3 Frequency characteristics of operational amplifiers that can be used with unity gain
Fig. 4 General amplifier circuit using operational amplifier
Fig. 4 General amplifier circuit using operational amplifier

Operational amplifiers (op-amps) are commonly used in two main types of amplification circuits: inverting amplifiers and non-inverting amplifiers. The voltage follower, also known as a unity gain amplifier, falls into the category of non-inverting amplifiers. In a voltage follower, the gain of the non-inverting amplifier is set to 0 dB (with (R_1 = 0) and (R_2 = ∞)).

Here’s how these two types of amplifiers work:

Non-Inverting Amplifier:

  • In a non-inverting amplifier, the input is applied to the positive terminal, and feedback is taken from the negative terminal.
  • Since the input is connected to the positive side of the op-amp, the phase starts at 0° (similar to the frequency response of a standalone op-amp).
  • As the frequency increases, the phase shift progresses from 0° to +180°.

Inverting Amplifier:

  • In an inverting amplifier, the input is applied to the negative terminal, and feedback is taken from the output.

The phase shift in an inverting amplifier starts at +180° and decreases as the frequency increases.

The voltage follower is a full feedback non-inverting amplifier circuit with a feedback rate of 100%. It has a band with a gain of 0dB and a cutoff frequency fT. Since the output is fed back to the negative terminal to form negative feedback, if the phase is delayed by 180° within the band, positive feedback will occur at that frequency and oscillation will occur.
The phase of a voltage follower for an operational amplifier that does not guarantee unity gain and an operational amplifier that does guarantee unity gain is as follows. The phase lag is greatest at the cutoff frequency, for example in the figure below (Fig. 5), it is close to -180°, and there is almost no phase margin. (Depending on the product, it may be zero.) 
On the other hand, products with a guaranteed unity gain have a phase margin of 90°. (Fig. 6)
However, this is the situation when there is no capacitive load. In reality, there is an output capacitance of the operational amplifier, stray capacitance of wiring, and capacitance on the load side, so further phase lag may occur. Therefore, it can be said that there is a high possibility of oscillation occurring in products that do not have a guarantee of unity gain.

Even products that guarantee unity gain may oscillate if the load capacitance is large, if the cutoff frequency of the LPF consisting of the load capacitance and output impedance is lower than the operational amplifier's fT, or if it is located nearby.

Fig. 5 Frequency characteristics of an operational amplifier that cannot achieve unity gain (Voltage follower)
Fig. 5 Frequency characteristics of an operational amplifier that cannot achieve unity gain (Voltage follower)
Fig. 6 Frequency characteristics of operational amplifiers that can be used with unity gain (Voltage follower)
Fig. 6 Frequency characteristics of operational amplifiers that can be used with unity gain (Voltage follower)

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