Exercise 3.7Z: Partial Fraction Decomposition
In the graph, four two-port networks are given by their pole–zero diagrams HL(p) .
- They all have in common that the number Z of zeros is equal to the number N of poles.
- The constant factor in each case is K=1.
In the special case Z=N the residue theorem cannot be applied directly to compute the impulse response h(t) .
Rather, a partial fraction decomposition corresponding to
- HL(p)=1−HL′(p)
must be made beforehand. Then,
- h(t)=δ(t)−h′(t) holds for the impulse response.
h′(t) is the inverse Laplace transform of HL′(p) , where the condition Z′<N′ is satisfied.
Two of the four configurations given are so-called all-pass filters.
- This refers to two-port networks for which the Fourier spectral function satisfies the condition |H(f)|=1 ⇒ a(f)=0 .
- In Exercise 3.4Z it is given how the poles and zeros of such an all-pass filter must be positioned.
Furthermore, in this exercise the p–transfer function
- H(5)L(p)=p/A(√p/A+√A/p)2
⇒ "configuration (5)" will be examined in more detail, which can be represented by one of the four pole–zero diagrams given in the graph if the parameter A is chosen correctly.
Please note:
- The exercise belongs to the chapter Inverse Laplace Transform.
- In particular, reference is made to the page Partial fraction decomposition.
Questions
Solution
- According to the criteria given in exercise 3.4Z, there is always an all-pass filter at hand if there is a corresponding zero po=+A+j⋅B in the right p–half-plane for each pole px=−A+j⋅B in the left half-plane.
- Considering K=1 the attenuation function is then a(f)=0 Np ⇒ |H(f)|=1.
- The following can be seen from the graph on the information page: The configurations (1) and (2) satisfy exactly these symmetry properties.
(2) The suggested solution 4 is correct:
- The transfer function H(5)L(p) is also described by configuration (4) as the following calculation shows:
- H(5)L(p)=p/A(√p/A+√A/p)2=p/Ap/A+2+A/p=p2p2+2A⋅p+A2=p2(p+A)2=H(4)L(p).
- The double zero is at po=0 and the double pole at px=−A=−2.
(3) The following holds for configuration (1) :
- HL(p)=p−2p+2=p+2−4p+2=1−4p+2=1−HL′(p)⇒HL′(p)=4p+2⇒HL′(p=0)=2_.
(4) Similarly, the following is obtained for configuration (2):
- HL(p)=(p−2−j⋅2)(p−2+j⋅2)(p+2−j⋅2)(p+2+j⋅2)=p2−4⋅p+8p2+4⋅p+8=p2+4⋅p+8−8⋅pp2+4⋅p+8=1−8⋅pp2+4⋅p+8=1−HL′(p)
- ⇒HL′(p)=8⋅p(p+2−j⋅2)(p+2+j⋅2).
Thus, the suggested solutions 2 and 3 are correct in contrast to statement 1:
- While HL(p) has two conjugate complex zeros,
- HL′(p) only has a single zero at po′=0.
(5) The following applies for Konfiguration (3) :
- HL(p)=p2p2+4⋅p+8=p2+4⋅p+8−4⋅p−8p2+4⋅p+8=1−HL′(p)
- ⇒HL′(p)=4⋅p+2(p+2−j⋅2)(p+2+j⋅2).
- The zero of HL′(p) is now at po′=−2.
- The constant is K′=4 ⇒ only suggested solution 2 is correct here.
(6) Finally, the following holds for configuration (4):
- HL(p)=p2(p+2)2=p2+4⋅p+4−4⋅p−4p2+4⋅p+4=1−4⋅p+4p2+4⋅p+4⇒HL′(p)=4⋅p+1(p+2)2.
Suggested solution 2 is also correct here. In general, it can be said that:
- The partial fraction decomposition changes the number and position of the zeros.
- On the contrary, the poles of HL′(p) are always identical to those of HL(p).