Difference between revisions of "Aufgaben:Exercise 3.7Z: Partial Fraction Decomposition"
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[[File:P_ID1789__LZI_Z_3_7.png|right|frame|Pole-zero diagrams]] | [[File:P_ID1789__LZI_Z_3_7.png|right|frame|Pole-zero diagrams]] | ||
− | In the graph, four two-port networks are given by their pole–zero diagrams HL(p) | + | 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. | * 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. | *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) | + | 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 | + | Rather, a "partial fraction decomposition" corresponding to |
:$$H_{\rm L}(p) =1- H_{\rm L}\hspace{0.05cm}'(p) | :$$H_{\rm L}(p) =1- H_{\rm L}\hspace{0.05cm}'(p) | ||
\hspace{0.05cm}$$ | \hspace{0.05cm}$$ | ||
must be made beforehand. Then, | must be made beforehand. Then, | ||
:$$h(t) = \delta(t)- h\hspace{0.03cm}'(t) | :$$h(t) = \delta(t)- h\hspace{0.03cm}'(t) | ||
− | \hspace{0.05cm}$$ holds for the impulse response. | + | \hspace{0.05cm}$$ |
− | h′(t) is the inverse Laplace transform of HL′(p) | + | 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 | + | Two of the four configurations given are so-called "all-pass filters". |
− | *This refers to two-port networks for which the Fourier | + | *This refers to two-port networks for which the Fourier spectrum satisfies the condition |H(f)|=1 ⇒ a(f)=0 . |
*In [[Aufgaben:Exercise_3.4Z:_Various_All-Pass_Filters|Exercise 3.4Z]] it is given how the poles and zeros of such an all-pass filter must be positioned. | *In [[Aufgaben:Exercise_3.4Z:_Various_All-Pass_Filters|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 | + | Furthermore, in this exercise the p–transfer function |
:$$H_{\rm L}^{(5)}(p) =\frac{p/A}{\left (\sqrt{p/A}+\sqrt{A/p} \right )^2} | :$$H_{\rm L}^{(5)}(p) =\frac{p/A}{\left (\sqrt{p/A}+\sqrt{A/p} \right )^2} | ||
\hspace{0.05cm}$$ | \hspace{0.05cm}$$ | ||
− | ⇒ "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. | + | ⇒ "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. |
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− | + | Please note: | |
*The exercise belongs to the chapter [[Linear_and_Time_Invariant_Systems/Inverse_Laplace_Transform|Inverse Laplace Transform]]. | *The exercise belongs to the chapter [[Linear_and_Time_Invariant_Systems/Inverse_Laplace_Transform|Inverse Laplace Transform]]. | ||
*In particular, reference is made to the page [[Linear_and_Time_Invariant_Systems/Inverse_Laplace_Transform#Partial_fraction_decomposition|Partial fraction decomposition]]. | *In particular, reference is made to the page [[Linear_and_Time_Invariant_Systems/Inverse_Laplace_Transform#Partial_fraction_decomposition|Partial fraction decomposition]]. | ||
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− | {Which | + | {Which two-port network has the transfer function H(5)L(p)? |
|type="()"} | |type="()"} | ||
- Configuration (1), | - Configuration (1), | ||
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− | {Compute the function HL′(p) after a partial fraction decomposition for configuration '''(1)'''. | + | {Compute the function HL′(p) after a partial fraction decomposition for configuration '''(1)'''. Enter the function value for p=0. |
|type="{}"} | |type="{}"} | ||
HL′(p=0) = { 2 3% } | HL′(p=0) = { 2 3% } | ||
− | {Compute HL′(p) for | + | {Compute HL′(p) for configuration (2). Which statements are true here? |
|type="[]"} | |type="[]"} | ||
- HL′(p) has the same zeros as HL(p). | - HL′(p) has the same zeros as HL(p). | ||
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− | {Compute HL′(p) for | + | {Compute HL′(p) for configuration (3). Which statements are true here? |
|type="[]"} | |type="[]"} | ||
- HL′(p) has the same zeros as HL(p). | - HL′(p) has the same zeros as HL(p). | ||
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− | {Compute HL′(p) for | + | {Compute HL′(p) for configuration (4). Which statements are true here? |
|type="[]"} | |type="[]"} | ||
- HL′(p) has the same zeros as HL(p). | - HL′(p) has the same zeros as HL(p). | ||
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===Solution=== | ===Solution=== | ||
{{ML-Kopf}} | {{ML-Kopf}} | ||
− | '''(1)''' The <u> suggested solutions 1 and 2</u> are correct: | + | '''(1)''' The <u> suggested solutions 1 and 2</u> are correct: |
− | *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. | + | *According to the criteria given in exercise 3.4Z, there is always an all-pass filter at hand <br>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. | *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. | *The following can be seen from the graph on the information page: The configurations (1) and (2) satisfy exactly these symmetry properties. | ||
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− | '''(2)''' The <u> suggested solution 4</u> is correct: | + | '''(2)''' The <u> suggested solution 4</u> is correct: |
*The transfer function H(5)L(p) is also described by configuration (4) as the following calculation shows: | *The transfer function H(5)L(p) is also described by configuration (4) as the following calculation shows: | ||
:$$H_{\rm L}^{(5)}(p) \hspace{0.25cm} = \hspace{0.2cm} \frac{p/A}{(\sqrt{p/A}+\sqrt{A/p})^2} | :$$H_{\rm L}^{(5)}(p) \hspace{0.25cm} = \hspace{0.2cm} \frac{p/A}{(\sqrt{p/A}+\sqrt{A/p})^2} | ||
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}= H_{\rm L}^{(4)}(p) | }= H_{\rm L}^{(4)}(p) | ||
\hspace{0.05cm}.$$ | \hspace{0.05cm}.$$ | ||
− | *The double zero is at po=0 and the double pole at px=−A=−2. | + | *The double zero is at po=0 and the double pole at px=−A=−2. |
− | '''(3)''' The following holds for configuration (1) | + | '''(3)''' The following holds for configuration (1): |
:$$H_{\rm L}(p) =\frac{p-2}{p+2}=\frac{p+2-4}{p+2}= 1 - \frac{4}{p+2}=1- H_{\rm L}\hspace{-0.05cm}'(p) | :$$H_{\rm L}(p) =\frac{p-2}{p+2}=\frac{p+2-4}{p+2}= 1 - \frac{4}{p+2}=1- H_{\rm L}\hspace{-0.05cm}'(p) | ||
\hspace{0.3cm} \Rightarrow \hspace{0.3cm}H_{\rm L}\hspace{-0.05cm}'(p) = \frac{4}{p+2} | \hspace{0.3cm} \Rightarrow \hspace{0.3cm}H_{\rm L}\hspace{-0.05cm}'(p) = \frac{4}{p+2} | ||
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− | '''(4)''' | + | '''(4)''' Similarly, the following is obtained for configuration (2): |
:$$H_{\rm L}(p) =\frac{(p-2 - {\rm j} \cdot 2)(p-2 + {\rm j} \cdot 2)}{(p+2 - {\rm j} \cdot 2)(p+2 + {\rm j} \cdot 2)}= | :$$H_{\rm L}(p) =\frac{(p-2 - {\rm j} \cdot 2)(p-2 + {\rm j} \cdot 2)}{(p+2 - {\rm j} \cdot 2)(p+2 + {\rm j} \cdot 2)}= | ||
\frac{p^2 -4\cdot p +8 }{p^2 +4\cdot p +8}= | \frac{p^2 -4\cdot p +8 }{p^2 +4\cdot p +8}= | ||
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\hspace{0.05cm}.$$ | \hspace{0.05cm}.$$ | ||
− | + | Thus, the <u> suggested solutions 2 and 3</u> 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)''' | + | '''(5)''' The following applies for configuration (3) : |
:$$H_{\rm L}(p) = | :$$H_{\rm L}(p) = | ||
\frac{p^2 }{p^2 +4\cdot p +8}=\frac{p^2 +4\cdot p +8 -4\cdot p -8 }{p^2 +4\cdot p +8} | \frac{p^2 }{p^2 +4\cdot p +8}=\frac{p^2 +4\cdot p +8 -4\cdot p -8 }{p^2 +4\cdot p +8} | ||
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\cdot \frac{p+2}{(p+2 - {\rm j} \cdot 2)(p+2 + {\rm j} \cdot 2)} | \cdot \frac{p+2}{(p+2 - {\rm j} \cdot 2)(p+2 + {\rm j} \cdot 2)} | ||
\hspace{0.05cm}.$$ | \hspace{0.05cm}.$$ | ||
− | * | + | *The zero of HL′(p) is now at po′=−2. |
− | * | + | *The constant is K′=4 ⇒ only <u> suggested solution 2</u> is correct here. |
− | '''(6)''' | + | '''(6)''' Finally, the following holds for configuration (4): |
:$$H_{\rm L}(p) = \frac{p^2 }{(p+2)^2}=\frac{p^2 +4\cdot p +4 -4\cdot p -4 }{p^2 +4\cdot p +4} | :$$H_{\rm L}(p) = \frac{p^2 }{(p+2)^2}=\frac{p^2 +4\cdot p +4 -4\cdot p -4 }{p^2 +4\cdot p +4} | ||
= 1- \frac{4\cdot p +4 }{p^2 +4\cdot p +4} | = 1- \frac{4\cdot p +4 }{p^2 +4\cdot p +4} | ||
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\cdot \frac{p+1}{(p+2)^2} | \cdot \frac{p+1}{(p+2)^2} | ||
\hspace{0.05cm}.$$ | \hspace{0.05cm}.$$ | ||
− | + | <u>Suggested solution 2</u> is 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). |
{{ML-Fuß}} | {{ML-Fuß}} | ||
Latest revision as of 15:55, 25 January 2022
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 spectrum 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 configuration (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 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).