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Passive, active, and digital filters (3ed., CRC, 2009) - tiera.ru

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23-18 <strong>Passive</strong>, Active, <strong>and</strong> Digital FiltersH S (z 1 , z 2 ) ¼ H A (z 1 , z 2 ) [H SL (z 1 , z 2 )] 2(b) Decomposition of H 24 (z 1 , z 2 ): Similarly, H 24 (z 1 , z 2 ) can be decomposed into the cascade of atwo quadrant filter G 24 (z 1 , z 2 ) [as is shown in Figure 23.7b], <strong>and</strong> a b<strong>and</strong>pass filter H B (z 1 , z 2 )which can be realized by using two 1-D b<strong>and</strong>pass <strong>filters</strong> for both directions.H 24 (z 1 , z 2 ) ¼ G 24 (z 1 , z 2 )H B (z 1 , z 2 )The final configuration of the desired filter H(z 1 , z 2 ) is illustrated in Figure 23.12d, with thefinal transfer function being of the formH(z 1 , z 2 ) ¼ H 13 (z 1 , z 2 ) þ H 24 (z 1 , z 2 ) H 13 (z 1 , z 2 )H 24 (z 1 , z 2 )where the purpose of the term H 13 (z 1 , z 2 )H 24 (z 1 , z 2 ), is to remove the overlap that may becreated by adding H 13 (z 1 , z 2 ) <strong>and</strong> H 24 (z 1 , z 2 ).(2) Design of all the sub<strong>filters</strong>: At this point, the problem is to derive the two quadrant sub<strong>filters</strong>G 13 (z 1 , z 2 ) <strong>and</strong> G 24 (z 1 , z 2 ), the low-pass sub<strong>filters</strong> H L (z 1 , z 2 ) <strong>and</strong> H SL (z 1 , z 2 ), the allpass subfilterH A (z 1 , z 2 ), <strong>and</strong> the b<strong>and</strong>stop filter H B (z 1 , z 2 ).Note the symmetry of the given characteristics, the identical 1-D sections can be used todevelop all the above 2-D sub<strong>filters</strong>, <strong>and</strong> the given specifications can easily be combined intothe designs of all the 1-D sections.(3) By connecting all the 2-D sub<strong>filters</strong> in cascade or parallel as specified in Figure 23.12d, therequired 2-D filter is obtained. The 3-D plot of the amplitude response of the final resulting 2-D filter is depicted in Figure 23.12e.23.4 Design of Circularly Symmetric Filters23.4.1 Design of LP FiltersAs mentioned in Section 23.2.1, rotated <strong>filters</strong> can be used to design circularly symmetric <strong>filters</strong>. Costa <strong>and</strong>Venetsanopoulos [14] <strong>and</strong> Goodman [15] proposed two methods of this class, based on transforming ananalog transfer function or a discrete one by rotated filter transformation, respectively. The two methodslead to <strong>filters</strong> that are, theoretically, unstable but by using an alternative transformation suggested byMendonca et al. [16], this problem can be eliminated.23.4.1.1 Design Based on 1-D Analog Transfer FunctionCosta <strong>and</strong> Venetsanopoulos [14] proposed a method to design circularly symmetric <strong>filters</strong>. In their method,a set of 2-D analog transfer functions is first obtained by applying the rotated filter transformation inEquation 23.9a for several different values of the rotation angle b to a 1-D analog low-pass transferfunction. A set of 2-D discrete low-pass functions are then deduced through the application of the bilineartransformation. The design is completed by cascading the set of 2-D <strong>digital</strong> <strong>filters</strong> obtained. The stepsinvolved are as follows.Step 1. Obtain a stable 1-D analog low-pass transfer functionH Al (s) ¼ Ns Q MDs ¼ K i¼1 (s0 Q Ni¼1 (sz ai)p ai)(23:50)wherez ai <strong>and</strong> p ai for i ¼ 1, 2, . . . , are the zeros <strong>and</strong> poles of H A1 (s), respectivelyK 0 is a multiplier constant

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