The circuit shows two cascaded identical second-order Sallen-Key low-pass filter stages. The overall filter is fourth-order.
For a Sallen-Key low-pass filter with equal resistors (R) and equal capacitors (C) in the RC network part (as shown in each stage: R = 1k\(\Omega\), C = 0.16\(\mu\)F for the frequency determining part), the natural frequency or characteristic frequency (\(f_c\) or \(f_0\)) of each second-order stage is given by:
\[ f_c = \frac{1}{2\pi RC} \]
Given:
R = 1 k\(\Omega\) = \(1 \times 10^3 \Omega\)
C = 0.16 \(\mu\)F = \(0.16 \times 10^{-6}\) F
Calculate \(f_c\) for one stage:
\[ f_c = \frac{1}{2\pi (1 \times 10^3 \Omega)(0.16 \times 10^{-6} \text{ F})} \]
\[ f_c = \frac{1}{2\pi (0.16 \times 10^{-3})} = \frac{1}{2\pi \times 0.00016} \]
\[ f_c = \frac{1}{0.0010053} \approx \frac{1}{0.001} \text{ Hz} = 1000 \text{ Hz} = 1 \text{ kHz} \]
Let's calculate more precisely:
\(RC = 10^3 \times 0.16 \times 10^{-6} = 0.16 \times 10^{-3} = 1.6 \times 10^{-4}\)
\(f_c = \frac{1}{2\pi \times 1.6 \times 10^{-4}} = \frac{10^4}{3.2\pi}\)
\(3.2\pi \approx 3.2 \times 3.14159 \approx 10.053\)
\(f_c \approx \frac{10000}{10.053} \approx 994.7 \text{ Hz}\).
This is very close to 1 kHz.
The gain of each non-inverting amplifier stage is \(K = 1 + R_2/R_1\). Here \(R_1 = 10\text{k}\Omega\) and \(R_2 = 12.35\text{k}\Omega\).
\(K = 1 + \frac{12.35 \text{k}\Omega}{10 \text{k}\Omega} = 1 + 1.235 = 2.235\). This gain affects the Q-factor and damping of the filter stage (e.g., for a Butterworth response, K is specific, usually 1.586 for Q=0.707).
However, the "cut off frequency" usually refers to the -3dB frequency, which for many standard filter designs (like Butterworth) is very close to the characteristic frequency \(f_c = 1/(2\pi RC)\) for each stage if the stages are designed to have their -3dB points at this frequency.
If it's a cascade of two identical Butterworth stages each with cutoff \(f_c\), the overall -3dB cutoff frequency of the 4th order filter will be lower than \(f_c\). However, often \(f_c\) is what is quoted as "the cutoff frequency" in simple terms.
Given the options, 1 kHz is the most direct calculation from \(1/(2\pi RC)\).
For a 4th order Butterworth filter made by cascading two 2nd order stages, if the overall -3dB cutoff is \(f_{c,overall}\), then each stage is typically designed with a specific \(f_0\) and Q that are slightly different from \(f_{c,overall}\).
But if the question implies each stage has its characteristic frequency at \(1/(2\pi RC)\) and asks for *this* frequency as "the cut off frequency" (perhaps of the individual sections contributing to the overall response):
The calculation \(f_c \approx 994.7 \text{ Hz}\) is approximately 1 kHz.
The "cut off frequency" of the overall fourth-order filter will be this value (1kHz) if the design is such that each identical stage has its -3dB point at 1kHz and they are directly cascaded (assuming no loading effects or that the stages are buffered, which they are by op-amps). In such a cascade of identical low-pass stages, the overall -3dB cutoff frequency becomes lower.
However, it is common in such questions to ask for the characteristic frequency \(f_c = 1/(2\pi RC)\) of the individual identical stages.
Given the options, 1 kHz is the result of this calculation.
\[ \boxed{1 \text{ kHz}} \]