When we get a circuit such as the following:
How do we define the cut-off frequency? Is it still $$f_c = \frac1{2\pi R_1C_1}$$ since \$f_c\$ is defined for \$X_{c1} = R_1\$? Or is it defined so that \$V_{out}\$(the one after OA3) is \$0.707V_2\$?
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Sign up to join this communityWhen we get a circuit such as the following:
How do we define the cut-off frequency? Is it still $$f_c = \frac1{2\pi R_1C_1}$$ since \$f_c\$ is defined for \$X_{c1} = R_1\$? Or is it defined so that \$V_{out}\$(the one after OA3) is \$0.707V_2\$?
The cutoff frequency is defined as the -3dB point, where 0dB is defined as the amplitude of the signal in the passband. So it's still \$\frac{1}{2πR_1 C_1}\$.
It's defined to be the half-power point. Since power is proportional to \$V^2\$ (and \$I^2\$ for that matter), one half power is when \$V_\text{OUT}=\frac{V_\text{IN}}{\sqrt{2}}\approx 0.7071\cdot V_\text{IN}\$.
There are other definitions. Different filter types may set the bar elsewhere (Chebyshev, for example.)
My own way of looking at it is that the critical point is when the \$2^\text{nd}\$ derivative of phase with respect to frequency goes through zero. But that's my arbitrary choice and it incorporates the effects of nearby poles and zeros. So just ignore me on that point.
How do we define the cutoff frequency in an active Op-Amp filter?
For a simple RC filter the so-called cut-off frequency is when the impedance of the capacitor equals the resistance of the resistor i.e.: -
\$\dfrac{1}{2\pi f C} = R\$
Re-arranging we get \$f = \dfrac{1}{2\pi C R}\$
In your circuit you do have op-amps but, they are only providing "gain" and this does not alter the relationship between cut-off frequency, C and R except in the case when the cut-off frequency is so high that the op-amps can no-longer provide that gain.