# Single Pole Op-AMP low pass Buffer

Note: This is a low pass amplifier/buffer. At high frequencies it has an effective  gain of one. If this is used as an amplifier it will have an effect of not amplifying the higher frequencies. Hence low pass buffer, not low pass filter!

![[NONINVLP_OPAMP_BUFFER.jpg]]
A single buffer op-amp, with $R_1$ to 
plus and $R_2$ as feedback, with a parallel feedback resistor, will act as a low pass filter with a 3Db cut-off point at,
$$ f_c = \frac{1}{2.\pi.R_2.C} \; .$$


The gain of the filter effect at frequency $f$ where the cut-off is $f_c$ is
$$|H| = \frac{1}{\sqrt{1+(\frac{f}{f_c})^2} + 1}$$

Note this is a single pole filter with a characteristic, past $f_c$ of
** Every *×10* increase in frequency → *–20 dB*
** Every *×2* increase in frequency → –6 dB
But in this case its drop off from the Gain of the amplifier. High frequencies will have a theoretical lowest gain of one.

A double pole actual low pass filter configuration is the [[Sallen Key]].

## Example

If $R_1$, $R_2$ are 22k and the capactor $C_1$ is 1nF the $3Db$ point will be 

$$ \frac{1}{2 \times \pi\times22E3\times1E-9} = 7.2E3$$ or 7.2kHz.

At 10 Mhz lets calculate the attenuation:-0=

$$ |H| = \frac{1}{\sqrt{1 +(\frac{10E6}{7.2E3})^2}} = \frac{1}{1388.9} = 720E{-6}$$

Converting this to $Amplitude \; Db$ i.e. $20  log_{10} (|H|)$  giving $-62.8 Db$
![[FB_IMG_1771442897824 3.jpg]]