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

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If one replaces the cosine function with the complex exponential function, one arrives at the analytical signal
If one replaces the cosine function with the complex exponential function, one arrives at the analytical signal
:$$s_{\rm +}(t) = s_0\cdot {\rm e}^{{\rm j}\hspace{0.05cm}\cdot \hspace{0.05cm}(
:$$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)) }.$$
\omega_{\rm T} \hspace{0.05cm}\cdot \hspace{0.05cm} t + \eta \hspace{0.05cm} \cdot \hspace{0.05cm} q(t)) }.$$
From this, one can calculate the equivalent low-pass signal sketched in the graph as follows:
From this, one can calculate the equivalent low-pass signal sketched in the graph as follows:
:$$s_{\rm TP}(t) = s_{\rm +}(t)  \cdot {\rm e}^{-{\rm
:$$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) }.$$
j}\hspace{0.05cm} \cdot\hspace{0.05cm} \omega_{\rm T} \hspace{0.05cm}\cdot\hspace{0.05cm}  t } = s_0\cdot
{\rm e}^{{\rm j}\hspace{0.05cm}\cdot\hspace{0.05cm} \eta \hspace{0.05cm} \cdot \hspace{0.05cm} q(t) }.$$




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'''(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 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&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.
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[[Category:Signal Representation: Exercises|^4.3 Equivalent LP Signal and its Spectral Function^]]
[[Category:Signal Representation: Exercises|^4.3 Equivalent LP Signal and its Spectral Function^]]
[[de:Aufgaben:Aufgabe 4.6Z: Ortskure bei Phasenmodulation]]

Latest revision as of 17:54, 16 March 2026

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  $t$.