Concept:
An RC phase shift oscillator uses an amplifier network combined with a feedback loop consisting of three identical RC sections. Each RC network section introduces a specific phase shift, and together the three sections create a total phase shift of exactly $180^\circ$ at the frequency of oscillation.
To achieve sustained oscillations, the system must meet the Barkhausen criterion:
• The total loop phase shift must be $0^\circ$ or $360^\circ$. Because the three RC stages contribute $180^\circ$, the amplifier must be an inverting configuration (providing another $180^\circ$).
• The magnitude of the loop gain must satisfy:
\[ |\beta A| \ge 1 \]
where $A$ represents the voltage gain of the active amplifier and $\beta$ represents the feedback factor of the passive RC network.
Step 1: Determining the feedback attenuation factor \(\beta\).
For a standard three-stage ladder RC network where all resistors have value $R$ and all capacitors have value $C$, the feedback transfer function can be derived using nodal analysis or mesh equations. The attenuation factor $\beta$ at the exact frequency where the phase shift is $180^\circ$ is found to be:
\[
\beta = \frac{1}{29}
\]
This means the output signal passing backward through the three RC network pairs is attenuated by a factor of 29.
Step 2: Calculating the minimum amplifier gain \(A\).
To maintain continuous, non-decaying sinusoidal oscillations, the total gain around the closed loop must be at least equal to unity:
\[
|A| \cdot |\beta| \ge 1
\]
Substituting the network attenuation factor $\beta = \frac{1}{29}$ into this condition:
\[
|A| \cdot \left(\frac{1}{29}\right) \ge 1
\]
Multiplying both sides by 29 gives:
\[
|A| \ge 29
\]
Therefore, the active amplifier configuration (such as a BJT common emitter or an op-amp inverting amplifier) must be set up to deliver a minimum voltage gain magnitude of 29 to compensate for the loss inside the feedback path.
Hence, the correct choice is option (3).