Hey guys, I am looking for some help in understanding the derivation for an n order butterworth filter.
Taken from wikipedia.org:
and hence,
I am sorry about the links not visible, if anyone could tell me how to make them visible i am all ears
Taken from wikipedia.org:
From above, it says that the poles of |H(jw)|^2 are evaluated. How is this correct? I dont understand the progression from magnitude squared expression to the actual transfer function. I guess the real prolem i have with it is this part and following:The transfer function
Plot of the gain of Butterworth low-pass filters of orders 1 through 5. Note that the slope is 20n dB/decade where n is the filter order.
Like all filters, the typical prototype is the low-pass filter, which can be modified into a high-pass filter, or placed in series with others to form band-pass and band-stop filters, and higher order versions of these.
The gain G(ω) of an n-order Butterworth low pass filter is given in terms of the transfer function H(s) as:
where
It can be seen that as n approaches infinity, the gain becomes a rectangle function and frequencies below ωc will be passed with gain G0, while frequencies above ωc will be suppressed. For smaller values of n, the cutoff will be less sharp.
- n = order of filter
- ωc = cutoff frequency (approximately the -3dB frequency)
- G0 is the DC gain (gain at zero frequency)
We wish to determine the transfer function H(s) where s = σ + jω. Since H(s)H(-s) evaluated at s = jω is simply equal to |H(jω)|2, it follows that:
The poles of this expression occur on a circle of radius ωc at equally spaced points. The transfer function itself will be specified by just the poles in the negative real half-plane of s. The k-th pole is specified by:
and hence,
The transfer function may be written in terms of these poles as:
The denominator is a Butterworth polynomial in s.
and hence,
I am sorry about the links not visible, if anyone could tell me how to make them visible i am all ears
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