\[
H(s) = A \cdot \frac{s^2 + \omega_0^2}{s^2 + \frac{\omega_0}{Q}s + \omega_0^2}
\]
\[
f_c = \frac{1}{2 \pi RC}
\]
\[
A = 1+\frac{R_A}{R_B}
\]
\[
BW = | f_c - f_{3db} |
\]
\[
H(s) = A \cdot \frac{s^2 + \omega_0^2}{s^2 + \frac{\omega_0}{Q}s + \omega_0^2}
\]
\[
f_c = \frac{1}{2 \pi RC}
\]
\[
A = 1+\frac{R_A}{R_B}
\]
\[
BW = | f_c - f_{3db} |
\]
| Fc [Hz] | |
| Amplitude [G/G] | |
| C [uF] | |
| 2C [uF] | |
| R [Ω] | |
| R/2 [Ω] | |
| RA [Ω] | |
| RB [Ω] | |
| result Fc0 [Hz] | |
| result BandWidth [Hz] | |
| result Gain at Fc [G/G] |