Filter Design Notes.
most of the notes taken will be derived from the 'Electronic Filter Design Handbook' second edition by Arthur B. Williams and Fred J. Taylor [its avalible on the internet archive]
most of the notes taken will be derived from the 'Electronic Filter Design Handbook' second edition by Arthur B. Williams and Fred J. Taylor [its avalible on the internet archive]
the general outline of a filter is that signals flow through it to a load, in a sense it is a black box where depending on the characteristics it can pass or attenuate signals.
For example a Low pass filter with unity gain with a corner frequency of 1kHz will allow signals below 1kHz to pass through unaffected, for frequencies at or greater than 1kHz they will start to be attenuated. At the corner frequency [-3dB] the signal strength is ~0.707X and the magnitude 'Rolls off' further as the frequency increases.
[Attenuated: meaning having been reduced in force, effect, etc.. in this case magnitude]
The Frequency response of a filter can be expressed as the ratio of two polynomials in terms of S.
S = jw, j = -1^0.5 and w = 2*pi*frequency
from figure 1-1, the output can be expressed as T(S) = E_load / E_source = N(s) / D(s)
The roots of the Denominator [D(S)] are called Poles
The roots of the Numerator [N(s)] are called Zeros
The example of T(s) in the top right shows a system that contains 3 poles and no Zeros IE, to be a pole or zero they must be a coefficient of S with an order >0
By plugging in S = jw to T(S) we can plot out the response of the filter across different frequencies
For a filter to work and be stable it must follow some mathematical rules, else it goes all wack.
when plotted on an axis with the X axis = real numbers [RE], Y axis = complex numbers [IM]
1) They must occur in pairs which are conjugates of each other, except for real-axis poles and zeros
2) Poles must also be restricted to the left plane, Zeroes may be present in either.