Difference between revisions of "Aufgaben:Exercise 4.6Z: Locality Curve for Phase Modulation"

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===Solution===
 
===Solution===
 
{{ML-Kopf}}
 
{{ML-Kopf}}
'''(1)'''   The locus curve is a circular arc with radius  $2$. Therefore, the magnitude function is constant   $\underline{a(t) = 2}$.
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'''(1)'''   The locality curve is a circular arc with radius  $2$.  Therefore, the magnitude function is constant   $\underline{a(t) = 2}$.
  
  
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'''(3)'''  In general, the relation  $s_{\rm TP}(t) = a(t) \cdot {\rm e}^{{\rm j}\hspace{0.05cm}\cdot \hspace{0.05cm}
 
'''(3)'''  In general, the relation  $s_{\rm TP}(t) = a(t) \cdot {\rm e}^{{\rm j}\hspace{0.05cm}\cdot \hspace{0.05cm}
\phi(t)}.$ applies here. A comparison with the given function yields:
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\phi(t)}$  applies here.  A comparison with the given function yields:
 
:$$\phi(t) = \eta \cdot q(t).$$
 
:$$\phi(t) = \eta \cdot q(t).$$
*The maximum phase value  $\phi_{\rm max} = +\pi \; \Rightarrow  \; {180^\circ}$  is obtained for the signal amplitude  $q_{\rm max} = 1$. From this follows directly  ${\eta = \pi} \; \underline{\approx 3.14}$.  
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*The maximum phase value  $\phi_{\rm max} = +\pi \; \Rightarrow  \; {180^\circ}$  is obtained for the signal amplitude  $q_{\rm max} = 1$.  From this follows directly  ${\eta = \pi} \; \underline{\approx 3.1415}$.  
 
*This modulation index is confirmed by the values  $\phi_{\rm min} = -\pi /2$  and  $q_{\rm min} = -0.5$ .
 
*This modulation index is confirmed by the values  $\phi_{\rm min} = -\pi /2$  and  $q_{\rm min} = -0.5$ .
  
  
[[File:P_ID769__Sig_Z_4_6_d_neu.png|right|frame|Locus curve (phase diagram) for a rectangular signal]]
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[[File:P_ID769__Sig_Z_4_6_d_neu.png|right|frame|Locality curve (phase diagram) for a rectangular source signal]]
 
'''(4)'''&nbsp;  <u>The second and third proposed solutions</u> are correct:
 
'''(4)'''&nbsp;  <u>The second and third proposed solutions</u> are correct:
 
*If&nbsp; $q(t) = \text{const.} =-0.5$, the phase function is also constant:
 
*If&nbsp; $q(t) = \text{const.} =-0.5$, the phase function is also constant:
 
:$$\phi(t) = \eta \cdot q(t) = - {\pi}/{2}\hspace{0.3cm}
 
:$$\phi(t) = \eta \cdot q(t) = - {\pi}/{2}\hspace{0.3cm}
 
\Rightarrow \hspace{0.3cm} s_{\rm TP}(t) = - {\rm j} \cdot s_0  = - 2{\rm j}.$$
 
\Rightarrow \hspace{0.3cm} s_{\rm TP}(t) = - {\rm j} \cdot s_0  = - 2{\rm j}.$$
*Thus, for the actual, physical signal:
+
*Thus, for the actual physical signal:
 
:$$s(t) = s_0 \cdot  {\cos} (  \omega_{\rm T}\hspace{0.05cm} t -
 
:$$s(t) = s_0 \cdot  {\cos} (  \omega_{\rm T}\hspace{0.05cm} t -
 
  {\pi}/{2}) = 2 \cdot  {\sin} (  \omega_{\rm T} \hspace{0.05cm} t ).$$
 
  {\pi}/{2}) = 2 \cdot  {\sin} (  \omega_{\rm T} \hspace{0.05cm} t ).$$
 
*In contrast,&nbsp; $q(t) = +0.5$&nbsp; leads to &nbsp;$\phi (t) = \pi /2$&nbsp; and to &nbsp;$s_{\rm TP}(t) = 2{\rm j}$.  
 
*In contrast,&nbsp; $q(t) = +0.5$&nbsp; leads to &nbsp;$\phi (t) = \pi /2$&nbsp; and to &nbsp;$s_{\rm TP}(t) = 2{\rm j}$.  
*If&nbsp; $q(t)$&nbsp; is a rectangular signal that alternates between&nbsp; $+0.5$&nbsp; and&nbsp; $–0.5$&nbsp; , then the locus curve consists of only two points on the imaginary axis, regardless of how long the intervals with &nbsp; $+0.5$&nbsp; and&nbsp; $–0.5$ last.
+
*If&nbsp; $q(t)$&nbsp; is a rectangular signal that alternates between&nbsp; $+0.5$&nbsp; and&nbsp; $–0.5$&nbsp; , then the locality curve consists of only two points on the imaginary axis, regardless of how long the intervals with &nbsp; $+0.5$&nbsp; and&nbsp; $–0.5$&nbsp; last.
 
*If, on the other hand,&nbsp; $q(t) = \pm 1$, then the possible phase values&nbsp; $+\pi$&nbsp; and&nbsp; $-\pi$ result purely formally, but they are identical.  
 
*If, on the other hand,&nbsp; $q(t) = \pm 1$, then the possible phase values&nbsp; $+\pi$&nbsp; and&nbsp; $-\pi$ result purely formally, but they are identical.  
*The „locus curve” then consists of only one point: &nbsp; $s_{\rm TP}(t) = - s_0$ &nbsp; <br>&rArr; &nbsp;  the signal&nbsp; $s(t)$&nbsp; is  „minus-cosine” for all times&nbsp; $t$&nbsp;.
+
*The locality curve then consists of only one point: &nbsp; $s_{\rm TP}(t) = - s_0$ &nbsp; &rArr; &nbsp;  the signal&nbsp; $s(t)$&nbsp; is&nbsp; "minus-cosine"&nbsp; for all times&nbsp; $t$.
  
  

Latest revision as of 15:02, 24 May 2021

A possible locality curve with phase modulation

We assume a source signal  $q(t)$, which is considered normalised.

  • The maximum value of this signal is  $q_{\rm max} = 1$  and the minimum signal value is  $q_{\rm min} = -0.5$.
  • Otherwise nothing is known about  $q(t)$.


The modulated signal with phase modulation   ⇒   "transmission signal"  is:

$$s(t) = s_0 \cdot {\cos} ( \omega_{\rm T}\hspace{0.05cm} t + \eta \cdot q(t)).$$

Here  $\eta$  denotes the so-called  "modulation index".  Let the constant envelope  $s_0$  also be a normalise quantity, which is set to  $s_0 = 2$  in the following (see diagram).

If one replaces the cosine function with the complex exponential function, one arrives at the analytical signal

$$s_{\rm +}(t) = s_0\cdot {\rm e}^{{\rm j}\hspace{0.05cm}\cdot \hspace{0.05cm}( \omega_{\rm T} \hspace{0.05cm}\cdot \hspace{0.05cm} t + \eta \hspace{0.05cm} \cdot \hspace{0.05cm} q(t)) }.$$

From this, one can calculate the equivalent low-pass signal sketched in the graph as follows:

$$s_{\rm TP}(t) = s_{\rm +}(t) \cdot {\rm e}^{-{\rm j}\hspace{0.05cm} \cdot\hspace{0.05cm} \omega_{\rm T} \hspace{0.05cm}\cdot\hspace{0.05cm} t } = s_0\cdot {\rm e}^{{\rm j}\hspace{0.05cm}\cdot\hspace{0.05cm} \eta \hspace{0.05cm} \cdot \hspace{0.05cm} q(t) }.$$



Hints:



Questions

1

What is the magnitude function  $a(t) = |s_{\rm TP}(t)|$?  Which value is valid for  $t = 0$?

$a(t = 0)\ = \ $

2

Between which extreme values  $\phi_{\rm min}$  and  $\phi_{\rm max}$  does the phase  $\phi (t)$?

$\phi_{\rm min}\ = \ $

 $\text{deg}$
$\phi_{\rm min}\ = \ $

 $\text{deg}$

3

Determine the modulation index  $\eta$  from the phase function  $\phi (t)$.

$\eta\ = \ $

4

Which of the following statements are true?

From  $q(t) = -0.5 = \text{const.}$  follows  $s(t) = s_0 \cdot \cos (\omega_T \cdot t)$.
With a rectangular signal  $($with only two possible signal values  $q(t)=\pm 0.5)$  the locality curve degenerates to two points.
With the signal values  $\pm 1$  $(q_{\rm min} = -0.5$  is then no longer valid$)$ the locality curve degenerates to one point:   $s_{\rm TP}(t) = -s_0$.


Solution

(1)  The locality curve is a circular arc with radius  $2$.  Therefore, the magnitude function is constant  $\underline{a(t) = 2}$.


(2)  From the graph it can be seen that the following numerical values apply:

  • $\phi_{\rm min} =- \pi /2 \; \Rightarrow \; \underline{-90^\circ}$,
  • $\phi_{\rm max} = +\pi \; \Rightarrow \; \underline{+180^\circ}$.


(3)  In general, the relation  $s_{\rm TP}(t) = a(t) \cdot {\rm e}^{{\rm j}\hspace{0.05cm}\cdot \hspace{0.05cm} \phi(t)}$  applies here.  A comparison with the given function yields:

$$\phi(t) = \eta \cdot q(t).$$
  • The maximum phase value  $\phi_{\rm max} = +\pi \; \Rightarrow \; {180^\circ}$  is obtained for the signal amplitude  $q_{\rm max} = 1$.  From this follows directly  ${\eta = \pi} \; \underline{\approx 3.1415}$.
  • This modulation index is confirmed by the values  $\phi_{\rm min} = -\pi /2$  and  $q_{\rm min} = -0.5$ .


Locality curve (phase diagram) for a rectangular source signal

(4)  The second and third proposed solutions are correct:

  • If  $q(t) = \text{const.} =-0.5$, the phase function is also constant:
$$\phi(t) = \eta \cdot q(t) = - {\pi}/{2}\hspace{0.3cm} \Rightarrow \hspace{0.3cm} s_{\rm TP}(t) = - {\rm j} \cdot s_0 = - 2{\rm j}.$$
  • Thus, for the actual physical signal:
$$s(t) = s_0 \cdot {\cos} ( \omega_{\rm T}\hspace{0.05cm} t - {\pi}/{2}) = 2 \cdot {\sin} ( \omega_{\rm T} \hspace{0.05cm} t ).$$
  • In contrast,  $q(t) = +0.5$  leads to  $\phi (t) = \pi /2$  and to  $s_{\rm TP}(t) = 2{\rm j}$.
  • If  $q(t)$  is a rectangular signal that alternates between  $+0.5$  and  $–0.5$  , then the locality curve consists of only two points on the imaginary axis, regardless of how long the intervals with   $+0.5$  and  $–0.5$  last.
  • If, on the other hand,  $q(t) = \pm 1$, then the possible phase values  $+\pi$  and  $-\pi$ result purely formally, but they are identical.
  • The locality curve then consists of only one point:   $s_{\rm TP}(t) = - s_0$   ⇒   the signal  $s(t)$  is  "minus-cosine"  for all times  $t$.