Aufgaben:Exercise 3.7Z: Partial Fraction Decomposition: Difference between revisions

From LNTwww
Nabil (talk | contribs)
Die Seite wurde neu angelegt: „ {{quiz-Header|Buchseite=Lineare zeitinvariante Systeme/Laplace–Rücktransformation }} right| :In der Grafik sind durch ih…“
 
Fix interlanguage link: resolve redirect chain
 
(37 intermediate revisions by 6 users not shown)
Line 1: Line 1:


{{quiz-Header|Buchseite=Lineare zeitinvariante Systeme/Laplace–Rücktransformation
{{quiz-Header|Buchseite=Linear_and_Time_Invariant_Systems/Inverse_Laplace_Transform
}}
}}


[[File:P_ID1789__LZI_Z_3_7.png|right|]]
[[File:P_ID1789__LZI_Z_3_7.png|right|frame|Pole-zero diagrams]]
:In der Grafik sind durch ihre Pol&ndash;Nullstellen&ndash;Diagramme <i>H</i><sub>L</sub>(<i>p</i>) vier verschiedene Vierpole gegeben. Sie alle haben gemein, dass die Anzahl <i>Z</i> der Nullstellen gleich der Anzahl <i>N</i> der Polstellen ist. Der konstante Faktor ist jeweils <i>K</i> = 1.
In the graph,&nbsp; four two-port networks are given by their pole&ndash;zero diagrams &nbsp;$H_{\rm L}(p)$.
* They all have in common that the number &nbsp;$Z$&nbsp; of zeros is equal to the number &nbsp;$N$&nbsp; of poles.  
*The constant factor in each case is &nbsp;$K=1$.


:Im Sonderfall <i>Z</i> = <i>N</i> kann zur Berechnung der Impulsantwort <i>h</i>(<i>t</i>) der Residuensatz nicht direkt angewendet werden. Vielmehr muss vorher eine Partialbruchzerlegung entsprechend
:$$H_{\rm L}(p)  =1- H_{\rm L}\hspace{0.05cm}'(p)
\hspace{0.05cm}$$
:vorgenommen werden. Für die Impulsantwort gilt dann
:$$h(t)  = \delta(t)- h\hspace{0.03cm}'(t)
\hspace{0.05cm},$$
:wobei <i>h</i>'(<i>t</i>) die Laplace&ndash;Transformierte von <i>H</i><sub>L</sub>'(<i>p</i>) angibt, bei der die Bedingung <i>Z</i>' < <i>N</i>' erfüllt ist.


:Bei zwei der vier angegebenen Konfigurationen handelt es sich um so genannte <i>Allpässe</i>. Darunter versteht man Vierpole, bei denen die Fourier&ndash;Spektralfunktion die Bedingung |<i>H</i>(<i>f</i>)| = 1 &nbsp;&#8658; a(<i>f</i>) = 0 erfüllt. In der Aufgabe Z3.4 ist angegeben, wie die Pole und Nullstelle eines solchen Allpasses angeordnet sein müssen.
In the special case &nbsp;$Z = N$&nbsp; the residue theorem cannot be applied directly to compute the impulse response &nbsp;$h(t)$.  


:Weiterhin soll in dieser Aufgabe die <i>p</i>&ndash;Übertragungsfunktion
Rather,&nbsp; a&nbsp; "partial fraction decomposition"&nbsp; corresponding to
:$$H_{\rm L}^{(5)}(p) =\frac{p/A}{\left (\sqrt{p/A}+\sqrt{A/p} \right )^2}
:$$H_{\rm L}(p) =1- H_{\rm L}\hspace{0.05cm}'(p)\hspace{0.05cm}$$
\hspace{0.05cm}$$
must be made beforehand. Then,
:näher untersucht werden, die bei richtiger Wahl des Parameters <i>A</i> durch eines der vier in der Grafik vorgegebenen Pol&ndash;Nullstellen&ndash;Diagramme dargestellt werden kann.
:$$h(t)  = \delta(t)- h\hspace{0.03cm}'(t)\hspace{0.05cm}$$
holds for the impulse response.
&nbsp;$h\hspace{0.03cm}'(t)$&nbsp; is the inverse Laplace transform of &nbsp;$H_{\rm L}\hspace{0.05cm}'(p)$,&nbsp; where the condition &nbsp;$Z' < N'$&nbsp; is satisfied.


:<b>Hinweis:</b> Die Aufgabe gehört zum Themengebiet von Kapitel 3.3.
Two of the four configurations given are so-called&nbsp; "all-pass filters".
*This refers to two-port networks for which the Fourier spectrum satisfies the condition &nbsp;$|H(f)| = 1$ &nbsp; &#8658; &nbsp; $a(f) = 0$&nbsp;.
*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.




===Fragebogen===
Furthermore,&nbsp; in this exercise the &nbsp;$p$&ndash;transfer function
:$$H_{\rm L}^{(5)}(p) =\frac{p/A}{\left (\sqrt{p/A}+\sqrt{A/p} \right )^2}\hspace{0.05cm}$$
&rArr; &nbsp; "configuration $(5)$" will be examined in more detail,&nbsp; which can be represented by one of the four pole&ndash;zero diagrams given in the graph if the parameter &nbsp;$A$&nbsp; is chosen correctly.
 
 
 
 
 
Please note:
*The exercise belongs to the chapter&nbsp;  [[Linear_and_Time_Invariant_Systems/Inverse_Laplace_Transform|Inverse Laplace Transform]].
*In particular, reference is made to the page&nbsp; [[Linear_and_Time_Invariant_Systems/Inverse_Laplace_Transform#Partial_fraction_decomposition|Partial fraction decomposition]].
 
 
 
===Questions===


<quiz display=simple>
<quiz display=simple>
{Bei welchen der skizzierten Vierpole handelt es sich um Allpässe?
{Which of the sketched two-port networks are all-pass filters?
|type="[]"}
|type="[]"}
+ Konfiguration (1),
+ Configuration &nbsp;$(1)$,
+ Konfiguration (2),
+ configuration &nbsp;$(2)$,
- Konfiguration (3),
- configuration &nbsp;$(3)$,
- Konfiguration (4).
- configuration &nbsp;$(4)$.




{Welcher Vierpol hat die Übertragungsfunktion <i>H</i><sub>L</sub><sup>(5)</sup>(<i>p</i>)?
{Which two-port network has the transfer function &nbsp;$H_{\rm L}^{(5)}(p)$?
|type="[]"}
|type="()"}
- Konfiguration (1),
- Configuration &nbsp;$(1)$,
- Konfiguration (2),
- configuration &nbsp;$(2)$,
- Konfiguration (3),
- configuration &nbsp;$(3)$,
+ Konfiguration (4).
+ configuration &nbsp;$(4)$.




{Berechnen Sie die Funktion <i>H</i><sub>L</sub>'(<i>p</i>) nach einer Partialbruchzerlegung für die Konfiguration (1). Geben Sie den Funktionswert für <i>p</i> = 0 ein.
{Compute the function &nbsp;$H_{\rm L}\hspace{0.01cm}'(p)$&nbsp; after a partial fraction decomposition for configuration&nbsp; '''(1)'''.&nbsp; Enter the function value for &nbsp;$p = 0$.
|type="{}"}
|type="{}"}
$Diagramm\ (1):\ \ H_L'(P = 0)$ = { 2 3% }
$H_{\rm L}\hspace{0.01cm}'(p = 0) \ = \ $ { 2 3% }




{Berechnen Sie <i>H</i><sub>L</sub>'(<i>p</i>) für Konfiguration (2). Welche Aussagen treffen hier zu?
{Compute &nbsp;$H_{\rm L}\hspace{0.01cm}'(p)$&nbsp; for configuration &nbsp;$(2)$.&nbsp; Which statements are true here?
|type="[]"}
|type="[]"}
- <i>H</i><sub>L</sub>'(<i>p</i>) besitzt die gleichen Nullstellen wie <i>H</i><sub>L</sub>(<i>p</i>).
- $H_{\rm L}\hspace{0.01cm}'(p)$&nbsp; has the same zeros as &nbsp;$H_{\rm L}(p)$.
+ <i>H</i><sub>L</sub>'(<i>p</i>) besitzt die gleichen Polstellen wie <i>H</i><sub>L</sub>(<i>p</i>).
+ $H_{\rm L}\hspace{0.01cm}'(p)$&nbsp; has the same poles as &nbsp;$H_{\rm L}(p)$.
+ Der konstante Faktor von <i>H</i><sub>L</sub>'(<i>p</i>) ist <i>K</i>' = 8.
+ The constant factor of &nbsp;$H_{\rm L}\hspace{0.01cm}'(p)$&nbsp; is &nbsp;$K' = 8$.




{Berechnen Sie <i>H</i><sub>L</sub>'(<i>p</i>) für Konfiguration (3). Welche Aussagen treffen hier zu?
{Compute &nbsp;$H_{\rm L}\hspace{0.01cm}'(p)$&nbsp; for configuration &nbsp;$(3)$.&nbsp; Which statements are true here?
|type="[]"}
|type="[]"}
- <i>H</i><sub>L</sub>'(<i>p</i>) besitzt die gleichen Nullstellen wie <i>H</i><sub>L</sub>(<i>p</i>).
- $H_{\rm L}\hspace{0.01cm}'(p)$&nbsp; has the same zeros as &nbsp;$H_{\rm L}(p)$.
+ <i>H</i><sub>L</sub>'(<i>p</i>) besitzt die gleichen Polstellen wie <i>H</i><sub>L</sub>(<i>p</i>).
+ $H_{\rm L}\hspace{0.01cm}'(p)$&nbsp; has the same poles as &nbsp;$H_{\rm L}(p)$.
- Der konstante Faktor von <i>H</i><sub>L</sub>'(<i>p</i>) ist <i>K</i>' = 8.
- The constant factor of &nbsp;$H_{\rm L}\hspace{0.01cm}'(p)$&nbsp; is &nbsp;$K' = 8$.




{Berechnen Sie <i>H</i><sub>L</sub>'(<i>p</i>) für Konfiguration (4). Welche Aussagen treffen hier zu?
{Compute &nbsp;$H_{\rm L}\hspace{0.01cm}'(p)$&nbsp; for configuration &nbsp;$(4)$.&nbsp; Which statements are true here?
|type="[]"}
|type="[]"}
- <i>H</i><sub>L</sub>'(<i>p</i>) besitzt die gleichen Nullstellen wie <i>H</i><sub>L</sub>(<i>p</i>).
- $H_{\rm L}\hspace{0.01cm}'(p)$&nbsp; has the same zeros as &nbsp;$H_{\rm L}(p)$.
+ <i>H</i><sub>L</sub>'(<i>p</i>) besitzt die gleichen Polstellen wie <i>H</i><sub>L</sub>(<i>p</i>).
+ $H_{\rm L}\hspace{0.01cm}'(p)$&nbsp; has the same poles as &nbsp;$H_{\rm L}(p)$.
- Der konstante Faktor von <i>H</i><sub>L</sub>'(<i>p</i>) ist <i>K</i>' = 8.
- The constant factor of &nbsp;$H_{\rm L}\hspace{0.01cm}'(p)$&nbsp; is &nbsp;$K' = 8$.




Line 72: Line 86:
</quiz>
</quiz>


===Musterlösung===
===Solution===
{{ML-Kopf}}
{{ML-Kopf}}
:<b>1.</b>&nbsp;&nbsp;Nach den in der Aufgabe Z3.4 angegebenen Kriterien liegt dann ein Allpass vor, wenn es zu jeder Polstelle <i>p</i><sub>x</sub> = &ndash; <i>A</i> + j &middot; <i>B</i> in der linken <i>p</i>&ndash;Halbebene eine entsprechende Nullstelle <i>p</i><sub>o</sub> = <i>A</i> + j &middot; <i>B</i> in der rechten Halbebene gibt. Mit <i>K</i> = 1 ist dann die Dämpfungsfunktion <i>a</i>(<i>f</i>) = 0 Np &nbsp;&#8658;&nbsp; |<i>H</i>(<i>f</i>)| = 1. Aus der Grafik auf der Angabenseite erkennt man, dass <u>die beiden Konfigurationen (1) und (2)</u> genau diese Symmetrieeigenschaften aufweisen.
'''(1)'''&nbsp; The&nbsp; <u> suggested solutions 1 and 2</u>&nbsp; are correct:
*According to the criteria given in exercise 3.4Z,&nbsp; there is always an all-pass filter at hand <br>if there is a corresponding zero &nbsp;$p_{\rm o} = + A + {\rm j} \cdot B$&nbsp; in the right $p$&ndash;half-plane for each pole &nbsp;$p_{\rm x} = - A + {\rm j} \cdot B$&nbsp; in the left half-plane.  
*Considering&nbsp; $K = 1$&nbsp; the attenuation function is then &nbsp;$a(f) = 0 \ \rm  Np$ &nbsp; &#8658; &nbsp; $|H(f)| = 1$.
*The following can be seen from the graph on the information page: &nbsp; The configurations &nbsp;$(1)$ and &nbsp;$(2)$ satisfy exactly these symmetry properties.
 
 
 
'''(2)'''&nbsp; The&nbsp; <u> suggested solution 4</u>&nbsp; is correct:
*The transfer function &nbsp;$H_{\rm L}^{(5)}(p)$&nbsp; is also described by configuration &nbsp;$(4)$&nbsp; as the following calculation shows:
:$$H_{\rm L}^{(5)}(p) \hspace{0.25cm} =  \hspace{0.2cm} \frac{p/A}{(\sqrt{p/A}+\sqrt{A/p})^2}=\frac{p/A}{{p/A}+2+ {A/p}}=  \hspace{0.2cm}\frac{p^2}{p^2 + 2A \cdot p + A^2} = \frac{p^2}{(p+A)^2}= H_{\rm L}^{(4)}(p)\hspace{0.05cm}.$$
*The double zero is at &nbsp;$p_{\rm o} = 0$&nbsp; and the double pole at &nbsp;$p_{\rm x} = -A = -2$.
 
 
 
'''(3)'''&nbsp; The following holds for configuration &nbsp;$(1)$:
:$$H_{\rm L}(p) =\frac{p-2}{p+2}=\frac{p+2-4}{p+2}= 1 - \frac{4}{p+2}=1- H_{\rm L}\hspace{-0.05cm}'(p)\hspace{0.3cm} \Rightarrow \hspace{0.3cm}H_{\rm L}\hspace{-0.05cm}'(p)  = \frac{4}{p+2}\hspace{0.3cm}\Rightarrow \hspace{0.3cm}\hspace{0.15cm}\underline{H_{\rm L}\hspace{-0.05cm}'(p =0)=2}\hspace{0.05cm}.$$
 
 
 
'''(4)'''&nbsp; Similarly,&nbsp; the following is obtained for configuration &nbsp;$(2)$:
:$$H_{\rm L}(p)  =\frac{(p-2 - {\rm j} \cdot 2)(p-2 + {\rm j} \cdot 2)}{(p+2 - {\rm j} \cdot 2)(p+2 + {\rm j} \cdot 2)}=\frac{p^2 -4\cdot p  +8 }{p^2 +4\cdot p  +8}=\hspace{0.2cm}\frac{p^2 +4\cdot p  +8 -8\cdot p}{p^2 +4\cdot p+8} =1- \frac{8\cdot p}{p^2 +4\cdot p  +8}=1- H_{\rm L}\hspace{-0.05cm}'(p)$$
:$$\Rightarrow \hspace{0.3cm}H_{\rm L}\hspace{0.05cm}'(p)  = 8\cdot \frac{p}{(p+2 - {\rm j} \cdot 2)(p+2 + {\rm j} \cdot 2)}\hspace{0.05cm}.$$
 
Thus,&nbsp; the&nbsp; <u> suggested solutions 2 and 3</u>&nbsp; are correct in contrast to statement 1:
* While &nbsp;$H_{\rm L}(p)$&nbsp; has two conjugate complex zeros,
* $H_{\rm L}\hspace{0.01cm}'(p)$&nbsp; only has a single zero at &nbsp;$p_{\rm o}\hspace{0.01cm}' = 0$.
 
 


:<b>2.</b>&nbsp;&nbsp;Die Übertragungsfunktion <i>H</i><sub>L</sub><sup>(5)</sup>(<i>p</i>) wird ebenso durch <u>die Konfiguration (4)</u> beschrieben, wie die nachfolgende Rechnung zeigt:
:$$H_{\rm L}^{(5)}(p) \hspace{0.25cm} =  \hspace{0.2cm} \frac{p/A}{(\sqrt{p/A}+\sqrt{A/p})^2}
=\frac{p/A}{{p/A}+2+ {A/p}}=\\
  =  \hspace{0.2cm}\frac{p^2}{p^2 + 2A \cdot p + A^2} = \frac{p^2}{(p+A)^2
}= H_{\rm L}^{(4)}(p)
\hspace{0.05cm}.$$
:Die beiden Nullstellen liegen bei <i>p</i><sub>o</sub> = 0, der doppelte Pol bei <i>p</i><sub>x</sub> = &ndash;<i>A</i> = &ndash;2.


:<b>3.</b>&nbsp;&nbsp;Für die Konfiguration (1) gilt:
'''(5)'''&nbsp; The following applies for configuration &nbsp;$(3)$&nbsp;:
:$$H_{\rm L}(p)  =\frac{p-2}{p+2}=\frac{p+2-4}{p+2}= 1 - \frac{4}{p+2}=1- H_{\rm L}\hspace{-0.05cm}'(p)$$
:$$H_{\rm L}(p)  =\frac{p^2 }{p^2 +4\cdot p  +8}=\frac{p^2 +4\cdot p  +8 -4\cdot p  -8 }{p^2 +4\cdot p +8}= 1- H_{\rm L}\hspace{-0.05cm}'(p)$$
:$$\Rightarrow \hspace{0.3cm}H_{\rm L}\hspace{-0.05cm}'(p)  = \frac{4}{p+2}
:$$\Rightarrow \hspace{0.3cm}H_{\rm L}\hspace{-0.05cm}'(p)  = 4\cdot \frac{p+2}{(p+2 - {\rm j} \cdot 2)(p+2 + {\rm j} \cdot 2)}\hspace{0.05cm}.$$
\hspace{0.3cm}\Rightarrow \hspace{0.3cm}\hspace{0.15cm}\underline{H_{\rm L}\hspace{-0.05cm}'(p =0)
*The zero of &nbsp;$H_{\rm L}\hspace{0.01cm}'(p)$&nbsp; is now at &nbsp;$p_{\rm o}\hspace{0.01cm}' = -2$.
=2}
*The constant is &nbsp;$K\hspace{0.01cm}' = 4$ &nbsp; &#8658; &nbsp; only &nbsp; <u> suggested solution 2</u> &nbsp; is correct here.
\hspace{0.05cm}.$$


:<b>4.</b>&nbsp;&nbsp;In gleicher Weise ergibt sich für die Konfiguration (2):
:$$H_{\rm L}(p)  \hspace{0.25cm} =  \hspace{0.2cm}\frac{(p-2 - {\rm j} \cdot 2)(p-2 + {\rm j} \cdot 2)}{(p+2 - {\rm j} \cdot 2)(p+2 + {\rm j} \cdot 2)}=
  \frac{p^2 -4\cdot p  +8 }{p^2 +4\cdot p  +8}=\\
  =  \hspace{0.2cm}\frac{p^2 +4\cdot p  +8 -8\cdot p}{p^2 -4\cdot p
+8}=1- \frac{8\cdot p}{p^2 +4\cdot p  +8}=1- H_{\rm L}\hspace{-0.05cm}'(p)$$
:$$\Rightarrow \hspace{0.3cm}H_{\rm L}\hspace{0.05cm}'(p)  = 8
\cdot \frac{p}{(p+2 - {\rm j} \cdot 2)(p+2 + {\rm j} \cdot 2)}
\hspace{0.05cm}.$$
:Richtig sind <u>die beiden letzten Lösungsvorschläge</u> im Gegensatz zur Aussage 1. Während <i>H</i><sub>L</sub>(<i>p</i>) zwei konjugiert&ndash;komplexe Nullstellen aufweist, besitzt <i>H</i><sub>L</sub>'(<i>p</i>) nur eine einzige Nullstelle bei <i>p</i> = 0.


:<b>5.</b>&nbsp;&nbsp;Für die Konfiguration (3) gilt:
:$$H_{\rm L}(p)  =
  \frac{p^2 }{p^2 +4\cdot p  +8}=\frac{p^2 +4\cdot p  +8 -4\cdot p  -8 }{p^2 +4\cdot p  +8}
= 1- H_{\rm L}\hspace{-0.05cm}'(p)$$
:$$\Rightarrow \hspace{0.3cm}H_{\rm L}\hspace{-0.05cm}'(p)  = 4
\cdot \frac{p+2}{(p+2 - {\rm j} \cdot 2)(p+2 + {\rm j} \cdot 2)}
\hspace{0.05cm}.$$
:Die Nullstelle von <i>H</i><sub>L</sub>'(<i>p</i>) liegt nun bei <i>p</i> = &ndash;2, die Konstante ist <i>K</i>' = 4 &#8658; richtig ist hier <u>nur Aussage 2</u>.


:<b>6.</b>&nbsp;&nbsp;Schließlich gilt für die Konfiguration (4):
'''(6)'''&nbsp; Finally,&nbsp; the following holds for configuration &nbsp;$(4)$:
:$$H_{\rm L}(p)  =  \frac{p^2 }{(p+2)^2}=\frac{p^2 +4\cdot p  +4 -4\cdot p  -4 }{p^2 +4\cdot p  +4}
:$$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}\hspace{0.3cm}\Rightarrow \hspace{0.3cm}H_{\rm L}\hspace{0.05cm}'(p)  = 4\cdot \frac{p+1}{(p+2)^2}\hspace{0.05cm}.$$
  = 1- \frac{4\cdot p  +4 }{p^2 +4\cdot p  +4}$$
<u>Suggested solution 2</u>&nbsp; is correct here.&nbsp; In general,&nbsp; it can be said that:  
:$$\Rightarrow \hspace{0.3cm}H_{\rm L}\hspace{0.05cm}'(p)  = 4
*The partial fraction decomposition changes the number and position of the zeros.  
\cdot \frac{p+1}{(p+2)^2}
* On the contrary,&nbsp; the poles of&nbsp; $H_{\rm L}\hspace{0.01cm}'(p)$&nbsp; are always identical to those of&nbsp; $H_{\rm L}(p)$.
\hspace{0.05cm}.$$
:Richtig ist auch hier <u>der Lösungsvorschlag 2</u>. Allgemein lässt sich sagen: Durch die Partialbruchzerlegung wird die Anzahl und die Lage der Nullstellen verändert. Die Pole von <i>H</i><sub>L</sub>'(<i>p</i>) sind dagegen stets identisch mit denen von <i>H</i><sub>L</sub>(<i>p</i>).
{{ML-Fuß}}
{{ML-Fuß}}






[[Category:Aufgaben zu Lineare zeitinvariante Systeme|^3.3 Laplace–Rücktransformation^]]
[[Category:Linear and Time-Invariant Systems: Exercises|^3.3 Inverse Laplace Transform^]]
[[de:Aufgaben:Aufgabe 3.7Z: Partialbruchzerlegung]]

Latest revision as of 17:57, 16 March 2026

Pole-zero diagrams

In the graph,  four two-port networks are given by their pole–zero diagrams  $H_{\rm L}(p)$.

  • 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

$$H_{\rm L}(p) =1- H_{\rm L}\hspace{0.05cm}'(p)\hspace{0.05cm}$$

must be made beforehand. Then,

$$h(t) = \delta(t)- h\hspace{0.03cm}'(t)\hspace{0.05cm}$$

holds for the impulse response.  $h\hspace{0.03cm}'(t)$  is the inverse Laplace transform of  $H_{\rm L}\hspace{0.05cm}'(p)$,  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

$$H_{\rm L}^{(5)}(p) =\frac{p/A}{\left (\sqrt{p/A}+\sqrt{A/p} \right )^2}\hspace{0.05cm}$$

⇒   "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.



Please note:



Questions

1 Which of the sketched two-port networks are all-pass filters?

Configuration  $(1)$,
configuration  $(2)$,
configuration  $(3)$,
configuration  $(4)$.

2 Which two-port network has the transfer function  $H_{\rm L}^{(5)}(p)$?

Configuration  $(1)$,
configuration  $(2)$,
configuration  $(3)$,
configuration  $(4)$.

3 Compute the function  $H_{\rm L}\hspace{0.01cm}'(p)$  after a partial fraction decomposition for configuration  (1).  Enter the function value for  $p = 0$.

$H_{\rm L}\hspace{0.01cm}'(p = 0) \ = \ $

4 Compute  $H_{\rm L}\hspace{0.01cm}'(p)$  for configuration  $(2)$.  Which statements are true here?

$H_{\rm L}\hspace{0.01cm}'(p)$  has the same zeros as  $H_{\rm L}(p)$.
$H_{\rm L}\hspace{0.01cm}'(p)$  has the same poles as  $H_{\rm L}(p)$.
The constant factor of  $H_{\rm L}\hspace{0.01cm}'(p)$  is  $K' = 8$.

5 Compute  $H_{\rm L}\hspace{0.01cm}'(p)$  for configuration  $(3)$.  Which statements are true here?

$H_{\rm L}\hspace{0.01cm}'(p)$  has the same zeros as  $H_{\rm L}(p)$.
$H_{\rm L}\hspace{0.01cm}'(p)$  has the same poles as  $H_{\rm L}(p)$.
The constant factor of  $H_{\rm L}\hspace{0.01cm}'(p)$  is  $K' = 8$.

6 Compute  $H_{\rm L}\hspace{0.01cm}'(p)$  for configuration  $(4)$.  Which statements are true here?

$H_{\rm L}\hspace{0.01cm}'(p)$  has the same zeros as  $H_{\rm L}(p)$.
$H_{\rm L}\hspace{0.01cm}'(p)$  has the same poles as  $H_{\rm L}(p)$.
The constant factor of  $H_{\rm L}\hspace{0.01cm}'(p)$  is  $K' = 8$.


Solution

(1)  The  suggested solutions 1 and 2  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  $p_{\rm o} = + A + {\rm j} \cdot B$  in the right $p$–half-plane for each pole  $p_{\rm x} = - A + {\rm j} \cdot B$  in the left half-plane.
  • Considering  $K = 1$  the attenuation function is then  $a(f) = 0 \ \rm Np$   ⇒   $|H(f)| = 1$.
  • 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  $H_{\rm L}^{(5)}(p)$  is also described by configuration  $(4)$  as the following calculation shows:
$$H_{\rm L}^{(5)}(p) \hspace{0.25cm} = \hspace{0.2cm} \frac{p/A}{(\sqrt{p/A}+\sqrt{A/p})^2}=\frac{p/A}{{p/A}+2+ {A/p}}= \hspace{0.2cm}\frac{p^2}{p^2 + 2A \cdot p + A^2} = \frac{p^2}{(p+A)^2}= H_{\rm L}^{(4)}(p)\hspace{0.05cm}.$$
  • The double zero is at  $p_{\rm o} = 0$  and the double pole at  $p_{\rm x} = -A = -2$.


(3)  The following holds for configuration  $(1)$:

$$H_{\rm L}(p) =\frac{p-2}{p+2}=\frac{p+2-4}{p+2}= 1 - \frac{4}{p+2}=1- H_{\rm L}\hspace{-0.05cm}'(p)\hspace{0.3cm} \Rightarrow \hspace{0.3cm}H_{\rm L}\hspace{-0.05cm}'(p) = \frac{4}{p+2}\hspace{0.3cm}\Rightarrow \hspace{0.3cm}\hspace{0.15cm}\underline{H_{\rm L}\hspace{-0.05cm}'(p =0)=2}\hspace{0.05cm}.$$


(4)  Similarly,  the following is obtained for configuration  $(2)$:

$$H_{\rm L}(p) =\frac{(p-2 - {\rm j} \cdot 2)(p-2 + {\rm j} \cdot 2)}{(p+2 - {\rm j} \cdot 2)(p+2 + {\rm j} \cdot 2)}=\frac{p^2 -4\cdot p +8 }{p^2 +4\cdot p +8}=\hspace{0.2cm}\frac{p^2 +4\cdot p +8 -8\cdot p}{p^2 +4\cdot p+8} =1- \frac{8\cdot p}{p^2 +4\cdot p +8}=1- H_{\rm L}\hspace{-0.05cm}'(p)$$
$$\Rightarrow \hspace{0.3cm}H_{\rm L}\hspace{0.05cm}'(p) = 8\cdot \frac{p}{(p+2 - {\rm j} \cdot 2)(p+2 + {\rm j} \cdot 2)}\hspace{0.05cm}.$$

Thus,  the  suggested solutions 2 and 3  are correct in contrast to statement 1:

  • While  $H_{\rm L}(p)$  has two conjugate complex zeros,
  • $H_{\rm L}\hspace{0.01cm}'(p)$  only has a single zero at  $p_{\rm o}\hspace{0.01cm}' = 0$.



(5)  The following applies for configuration  $(3)$ :

$$H_{\rm L}(p) =\frac{p^2 }{p^2 +4\cdot p +8}=\frac{p^2 +4\cdot p +8 -4\cdot p -8 }{p^2 +4\cdot p +8}= 1- H_{\rm L}\hspace{-0.05cm}'(p)$$
$$\Rightarrow \hspace{0.3cm}H_{\rm L}\hspace{-0.05cm}'(p) = 4\cdot \frac{p+2}{(p+2 - {\rm j} \cdot 2)(p+2 + {\rm j} \cdot 2)}\hspace{0.05cm}.$$
  • The zero of  $H_{\rm L}\hspace{0.01cm}'(p)$  is now at  $p_{\rm o}\hspace{0.01cm}' = -2$.
  • The constant is  $K\hspace{0.01cm}' = 4$   ⇒   only   suggested solution 2   is correct here.


(6)  Finally,  the following holds for configuration  $(4)$:

$$H_{\rm L}(p) = \frac{p^2 }{(p+2)^2}=\frac{p^2 +4\cdot p +4 -4\cdot p -4 }{p^2 +4\cdot p +4}= 1- \frac{4\cdot p +4 }{p^2 +4\cdot p +4}\hspace{0.3cm}\Rightarrow \hspace{0.3cm}H_{\rm L}\hspace{0.05cm}'(p) = 4\cdot \frac{p+1}{(p+2)^2}\hspace{0.05cm}.$$

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  $H_{\rm L}\hspace{0.01cm}'(p)$  are always identical to those of  $H_{\rm L}(p)$.