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The frequency response of a linear shift-invariant system may be found from the system function by evaluating H(z) on the unit circle. For a rational function of z, the frequency response may be found geometrically from the poles and zeros of H(z). With H(z) written in factored form as in Eq. (5.4), the frequency response is

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IH(ejW)lis IAl times the product of the terms I I - bke-jwl divided by the product of the terms 11 - ake-JWI. Each term in the numerator 11 - ,#ke-j"l = lejw - BkI is the length of the vector from the zero at z = Bk to the unit circle at z = ej" (labeled vl in Fig. 5-2). Similarly, each term in the denominator

hash(Rad) = 3, load = 9% hash(Uhr) = 4, load = 18% hash(Ohr) = 2, load = 27% hash(Tor) = 8, load = 36% hash(Hut) = 5, load = 45% 3, 4, 5, hash(Tag) = 6, load = 54%

private static void printHash(String word) { System.out.println("hash(" + word + ") = " + hash(word)); } private static int hash(Object object) { return (object.hashCode() & MASK) % CAPACITY; } }

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is the length of the vector from the pole at z = a k to the unit circle at z = ejw (labeled v2 in Fig. 5-2). When a pole is close to the unit circle, a k = rkejwk with r k = 1, the magnitude of the frequency response becomes large for w = w because the length of the vector from the pole to the unit circle becomes small. Similarly, if there is k with r k 1, the magnitude of the frequency response becomes small a zero close to the unit circle, Bk = rkeJWk k ~ ~ for w = w (if the zero is on the unit circle at z = ej"', ~ ( e j = 0). ) The analysis for the phase is similar. Assuming that A is a positive real number, the phase corresponding to the frequency response H (el") given by Eq. (5.7) is

CHAP. 8]

Thus, & ( a ) is the sum of the phases associated with the terms (1 - Bke-jw),minus the sum of the phases of the terms (1 - ake-Jw). Because . . 1 - pke-jo = e-Jw(eJw - B k

The output is:

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where 0, is the angle subtended by the vector from the zero at z = ,Ek to the unit circle at z = eJw(see Fig. 5-2). Similarly, for each term in the denominator

5, 6, hash(Eis) = 7, load = 63% 3, 4, 5, 6, 7, 8, hash(Ast) = 9, load = 72% 9, hash(Zug) = 10, load = 81% 3, 4, 5, 6, 7, 8, 9, 10, hash(Hof) = 0, load = 90% 2, 3, 4, 5, 6, 7, 8, 9, 10, 0, hash(Mal) = 1, load = 100% The size field contains the number of items hashed into the table. The used[] array flags which components are occupied in the table. The printHash() method prints the hash table index and the

hash(Rad) hash(Uhr) hash(Ohr) hash(Tor) hash(Hut) hash(Tag) = = = = = = 99 82 73 45 13 4

where Q2 is the angle of the vector from the pole at z = a!k to the unit circle at z = eJW.When a pole (zero) is close to the unit circle, the phase decreases (increases) rapidly as we move past the pole (zero). Because the group delay is the negative of the derivative of the phase, this implies that the group delay is large and positive close to a pole and large and negative when close to a zero.

A linear shift-invariant system is said to have linear phase if the frequency response has the form

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