Difference between revisions of "Bessel Filters"
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(Created page with " == The Low-Pass Bessel Filter ==") |
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+ | Bessel filters are ''all-pole filters'' with maximally flat pass-bands, ''maximally flat group delays'', and poor "out-of-band" or stop-band attenuation compared to Butterworth, Chebyshev, and Elliptic filters of the same order. Since the group delays are relatively constant in the pass-band, Bessel filters exhibit minimal phase distortion, and hence very little overshoot in its step response. | ||
+ | == The Low-Pass Bessel Filter == | ||
+ | The transfer function of the low-pass Bessel filter is given by: | ||
+ | |||
+ | {{NumBlk|::|<math> | ||
+ | H\left(s\right) = \frac{\theta_N\left(0\right)}{\theta_N\left(\frac{s}{\omega_0}\right)} | ||
+ | </math>|{{EquationRef|1}}}} | ||
+ | |||
+ | Where <math>N</math> is the filter order, <math>\omega_0</math> is the cut-off frequnecy, and <math>\theta_N\left(s\right)</math> is the reverse Bessel polynomial, and is equal to: | ||
− | == | + | {{NumBlk|::|<math> |
+ | \theta_N\left(s\right) = \sum_{k=0}^N a_k s^k | ||
+ | </math>|{{EquationRef|2}}}} | ||
+ | |||
+ | Where: | ||
+ | |||
+ | {{NumBlk|::|<math> | ||
+ | a_k =\frac{\left(2N-k\right)!}{2^{N-k}k!\left(N-k\right)!} | ||
+ | </math>|{{EquationRef|3}}}} | ||
+ | |||
+ | For <math>k=0,1,\ldots N</math>. |
Revision as of 01:43, 16 March 2021
Bessel filters are all-pole filters with maximally flat pass-bands, maximally flat group delays, and poor "out-of-band" or stop-band attenuation compared to Butterworth, Chebyshev, and Elliptic filters of the same order. Since the group delays are relatively constant in the pass-band, Bessel filters exhibit minimal phase distortion, and hence very little overshoot in its step response.
The Low-Pass Bessel Filter
The transfer function of the low-pass Bessel filter is given by:
-
(1)
-
Where is the filter order, is the cut-off frequnecy, and is the reverse Bessel polynomial, and is equal to:
-
(2)
-
Where:
-
(3)
-
For .