Hi,

Can anyone tell me how to calculate the cuttoff frequency and circuit delay in cascaded low pass RC filter.

1. Cuttoff frequency calculation
2. Equation for KCL in Laplace form for calcualting circuit delay

I have contacted many people, but i have not got the desired answer.
Please anyone help me in solving my problem.

I am attaching the schematic for your reference..

 

I get 's' domain transfer function .....

\(\frac{V_o}{V_i}=\frac{1}{R_1R_2C_1C_2\[s^2+\[\frac{1}{R_1C_1}+\frac{1}{R_2C_2}+\frac{1}{R_2C_1}\]s+\frac{1}{R_1R_2C_1C_2}\]}\)

Where R1, R2, C1 & C2 are from left to right on your schematic

which for your values gives cut-off at f0=1865.4 Hz [-9.134dB] based on ....

\(\omega_o^2=\frac{1}{R_1R_2C_1C_2}\)

The -3dB point is at about 753 Hz.

The rise time [10% to 90% FV] to a pulse input is about 478.7 uS - done by simulation.

 

Could you please explain me
How

and The -3dB point is at about 753 Hz.

I am able to understand how the below transfer function came

but not the first and second frequency

 

Could you please explain me
How

and The -3dB point is at about 753 Hz.

I am able to understand how the below transfer function came
Could you please explain me
How

and The -3dB point is at about 753 Hz.

I am able to understand how the below transfer function came

but not the first and second frequency

but not the first and second frequency

 

Could you please explain me
How

and The -3dB point is at about 753 Hz.

From the general 2nd order transfer function denominator term of the form

\(s^2+2\zeta\omega_o s+\omega_o^2\)

the phase shift is 90° at

\(\omega=\omega_o\)

where the substitution s=jω is made in the second order denominator term.

The assumption used is that the cut-off is defined at that value of ω where the transfer function phase shift value is 90°.

The 753 Hz -3dB is obtained by solving for the required ω value at the -3dB value for the transfer function magnitude.

It depends on what one defines as the cut-off frequency. The normal convention is to take the -3dB frequency. The issue is reconciling the mathematical interpretation with respect to the transfer function at the frequency ωo.

 

I tried this a few years ago, but eventually gave up and had to go to active filters. I actually built some 4th-order active lowpass filters (i.e. cascaded) using formulas from Horowitz' book. But eventually I found that even this didn't give sufficient "sharpness" of cut-off frequency. So I went to an off-the-shelf 8th-order Bessel filter. It's also programmable, allowing me to change the cutoff frequency digitally from 1 to 256 Hz...so it's pretty expensive. But they also make less glamorous 8th-order filters, etc. This was my experience, in a very condensed nutshell. Unless your application is able to handle an extremely "soft" knee or cut-off region, just cascading two passive filters together will not give good results.