Aufgaben:Exercise 3.5: PM and FM for Rectangular Signals: Difference between revisions

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{{quiz-Header|Buchseite=Modulationsverfahren/Frequenzmodulation (FM)
{{quiz-Header|Buchseite=Modulation_Methods/Frequency_Modulation_(FM)
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[[File:P_ID1099__Mod_A_3_5.png|right|]]
[[File:P_ID1099__Mod_A_3_5.png|right|frame|Two signal waveforms in angle modulation]]
Wir gehen von einem bipolaren und rechteckförmigen Quellensignal $q(t)$ aus, welches im oberen Diagramm dargestellt ist.
Assume a bipolar and rectangular source signal $q(t)$ , as shown in the upper diagram.  This signal can only take on the two signal values  $±A = ±2 \ \rm V$  and the duration of the positive and negative rectangles are each $T = 1 \ \rm ms$.  The period of  $q(t)$  is therefore   $T_0 = 2 \ \rm ms$.


Dieses kann nur die beiden Signalwerte $±A = ±2 V$ annehmen und die Dauer der positiven und negativen Rechtecke ist jeweils $T = 1 ms$. Die Periodendauer von $q(t)$ ist demzufolge $T_0 = 2 ms$.
The signals $s_1(t)$  and  $s_2(t)$  display two transmitted signals with angle modulation  $\rm (WM)$, each of which can be represented as
:$$s(t) = A_{\rm T} \cdot \cos \hspace{-0.05cm}\big [\psi (t) \big ]$$
Here, we distinguish between phase modulation  $\rm (PM)$  with the angular function
:$$\psi(t)  =  \omega_{\rm T} \cdot t + \phi(t)  = \omega_{\rm T} \cdot t + K_{\rm PM} \cdot q(t)$$
and frequency modulation  $\rm (FM)$, where the instantaneous freqiency is linearly related to $q(t)$:
:$$f_{\rm A}(t) = \frac{\omega_{\rm A}(t)}{2\pi}, \hspace{0.3cm} \omega_{\rm A}(t) = \frac{{\rm d}\hspace{0.03cm}\psi(t)}{{\rm d}t}= \omega_{\rm T} + K_{\rm FM} \cdot q(t)\hspace{0.05cm}.$$
$K_{\rm PM}$  and  $K_{\rm FM}$  denote the dimensionally constrained constants given by the realizations of the PM and FM modulators, respectively.  The frequency deviation  $Δf_{\rm A}$  indicates the maximum deviation of the instantaneous frequency from the carrier frequency.


Die Signale $s_1(t)$ und $s_2(t)$ zeigen zwei Sendesignale bei Winkelmodulation (WM), die jeweils in der Form
$$s(t) = A_{\rm T} \cdot \cos (\psi (t) )$$
darstellbar sind. Hierbei unterscheidet man zwischen der Phasenmodulation (PM) mit der Winkelfunktion
$$\psi(t)  =  \omega_{\rm T} \cdot t + \phi(t)$$
$$ =  \omega_{\rm T} \cdot t + K_{\rm PM} \cdot q(t)$$
und der Frequenzmodulation (FM), bei der die Augenblicksfrequenz linear mit $q(t)$ zusammenhängt:
$$f_{\rm A}(t) = \frac{\omega_{\rm A}(t)}{2\pi}, \hspace{0.3cm} \omega_{\rm A}(t) = \frac{{\rm d}\hspace{0.03cm}\psi(t)}{{\rm d}t}= \omega_{\rm T} + K_{\rm FM} \cdot q(t)\hspace{0.05cm}.$$
$K_{PM}$ und $K_{FM}$ bezeichnen dimensionsbehaftete, durch die Realisierung des PM– bzw. FM–Modulators vorgegebene Konstante. Der Frequenzhub $Δf_A$ gibt die maximale Abweichung der Augenblicksfrequenz von der Trägerfrequenz an.


'''Hinweis:''' Die Aufgabe bezieht sich auf die theoretischen Grundlagen von [http://en.lntwww.de/Modulationsverfahren/Phasenmodulation_(PM) Kapitel 3.1] und [http://en.lntwww.de/Modulationsverfahren/Frequenzmodulation_(FM) Kapitel 3.2]. Im Vorgriff auf das Kapitel 4 sei erwähnt, dass man die Phasenmodulation bei digitalem Eingangssignal auch als PSK (''Phase Shift Keying'') und entsprechend die Frequenzmodulation als FSK (''Frequency Shift Keying'') bezeichnet.


===Fragebogen===
 
 
 
 
 
''Hints:''
*This exercise belongs to the chapter  [[Modulation_Methods/Frequency_Modulation_(FM)|Frequency Modulation]].
*Reference is also made to the chapter   [[Modulation_Methods/Phase_Modulation_(PM)|Phase Modulation]].
*In anticipation of the fourth chapter, it should be mentioned that phase modulation with a digital input signal is also called ''Phase Shift Keying''  $\rm (PSK)$  and frequency modulation is analogously called ''Frequency Shift Keying''  $\rm (FSK)$ .
 
 
 
===Questions===


<quiz display=simple>
<quiz display=simple>
{Welches der Signale ist durch eine PM, welches durch eine FM entstanden?
{Which of the signals is due to phase modulation and which is due to frquency modulation?
|type="[]"}
|type="()"}
- $s_1(t)$ beschreibt eine Phasenmodulation.
- $s_1(t)$&nbsp; represents a phase modulation.
+ $s_1(t)$ beschreibt eine Frequenzmodulation.
+ $s_1(t)$&nbsp; represents a frequency modulation.


{Wie groß ist die Trägerphase $ϕ_T$, die man mit $q(t) = 0$ messen könnte?
{What is the carrier phase &nbsp;$ϕ_{\rm T}$ that could be measured without a message signal &nbsp; &rArr;  &nbsp; $q(t) \equiv 0$&nbsp;?
|type="{}"}
|type="{}"}
$ϕ_T$ = { 0 3% } $Grad$  
$ϕ_{\rm T} \ = \ $ { 0. } $\ \rm Grad$  


{Welche Trägerfrequenz (bezogen auf 1/T) wurde bei den Grafiken verwendet?
{What carrier frequency&nbsp; $($with respect to &nbsp;$1/T)$&nbsp; was used in the graphs?
|type="{}"}
|type="{}"}
$f_T · T$ = { 6 3% }  
$f_{\rm T} · T \ = \ $ { 6 3% }  


{Das Phase des PM–Signals ist $±90°$. Wie groß ist die Modulatorkonstante?
{The phase of the PM signal is &nbsp;$±90^\circ$.&nbsp; What is the modulator constant?
|type="{}"}
|type="{}"}
$K_{PM}$ = { 0.785 3% } $V^{-1}$  
$K_{\rm PM} \ = \ $ { 0.785 3% } $\ \rm V^{-1}$  


{Wie groß ist der Frequenzhub $Δf_A$ des FM–Signals, bezogen auf 1/T?
{What is the frequency deviation &nbsp;$Δf_{\rm A}$&nbsp; of the FM signal with respect to &nbsp;$1/T$?
|type="{}"}
|type="{}"}
$Δf_A · T$ = { 2 3% }  
$Δf_{\rm A} · T \ = \ $ { 2 3% }  


{Wie groß ist die FM–Modulatorkonstante?
{What is the FM modulator constant?
|type="{}"}
|type="{}"}
$K_{FM}$ = { 6283 3% } $(Vs)^{-1}$
$K_{\rm FM} \ = \ $ { 6283 3% } $\ \rm (Vs)^{-1}$




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</quiz>
</quiz>


===Musterlösung===
===Solution===
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'''1.''' Bei einem rechteckförmigen (digitalen) Quellensignal erkennt man die Phasenmodulation (PM) an den typischen Phasensprüngen siehe Signalverlauf $s_2(t)$. Die Frequenzmodulation (FM) weist dagegen zu den verschiedenen Zeiten unterschiedliche Augenblicksfrequenzen wie bei $s_1(t)$ auf ⇒ $\underline{Antwort 2}$.
'''(1)'''&nbsp; <u>Answer 2</u> is correct:
*For a rectangular (digital) source signal, phase modulation (PM) can be recognised by the typical phase jumps see the signal waveform&nbsp; $s_2(t)$.  
*Frequency modulation (FM), on the other hand, has diverse instantaneous frequencies at different times, as in&nbsp; $s_1(t)$.
 
 
 
'''(2)'''&nbsp;  When&nbsp; $q(t) = 0$&nbsp;, the equations provided for both PM and FM give
:$$s(t) = A_{\rm T} \cdot \cos (\omega_{\rm T} \cdot t ) \hspace{0.3cm}\Rightarrow\hspace{0.3cm} \phi_{\rm T} \hspace{0.15cm}\underline {= 0}\hspace{0.05cm}.$$
 
 
 
'''(3)'''&nbsp;  The carrier frequency&nbsp; $f_{\rm T}$&nbsp; can be directly determined only from the PM signal &nbsp; $s_2(t)$&nbsp;.
*By counting the oscillations of&nbsp; $s_2(t)$&nbsp; in the time interval&nbsp; $T$&nbsp;, it can be seen that&nbsp; $f_{\rm T} · T\hspace{0.15cm}\underline{ = 6}$&nbsp; was used.
*When frequency modulating a bipolar source signal, &nbsp; $f_{\rm T}$&nbsp; does not occur directly.
*However, the graphs do indicate that &nbsp;  $f_{\rm T} · T = 6$&nbsp; is also used here.
 




'''2.''' Mit $q(t) = 0$ erhält man entsprechend den gegebenen Gleichungen sowohl für PM als auch für FM
$$s(t) = A_{\rm T} \cdot \cos (\omega_{\rm T} \cdot t ) \hspace{0.3cm}\Rightarrow\hspace{0.3cm} \phi_{\rm T} \hspace{0.15cm}\underline {= 0}\hspace{0.05cm}.$$


'''(4)'''&nbsp;  The amplitude value&nbsp; $A = 2 \ \rm V$&nbsp; results in the phase&nbsp; $90^\circ$&nbsp; or&nbsp; $π/2$&nbsp; (minus sine wave).&nbsp; This gives:
:$$K_{\rm PM} = \frac {\pi /2}{2\,{\rm V}} \hspace{0.15cm}\underline {= 0.785\,{\rm V}^{-1}} \hspace{0.05cm}.$$


'''3.''' Die Trägerfrequenz $f_T$ kann direkt nur aus dem PM–Signal $s_2(t)$ ermittelt werden. Bei der FM eines bipolaren Quellensignals tritt $f_T$ nicht auf. Durch Abzählen der Schwingungen von $s_2(t)$ im Zeitintervall T erkennt man, dass $f_T · T = 6$ verwendet wurde.




'''4.''' Der Amplitudenwert $A = 2 V$ führt zur Phase $90°$ bzw. $π/2$ (Minus–Sinusverlauf). Daraus folgt:
'''(5)'''&nbsp;  The graph for&nbsp; $s_1(t)$&nbsp; shows that either four or eight oscillations arise within a time interval&nbsp; $T$&nbsp;: &nbsp; $4 \le f_{\rm A}(t) \cdot T \le 8\hspace{0.05cm}.$
$$K_{\rm PM} = \frac {\pi /2}{2\,{\rm V}} \hspace{0.15cm}\underline {= 0.785\,{\rm V}^{-1}} \hspace{0.05cm}.$
*Considering the (normalized) carrier frequency&nbsp; $f_{\rm T} · T = 6$&nbsp;, the (normalized) frequency deviation is:
:$$\Delta f_{\rm A} \cdot T \hspace{0.15cm}\underline {=2}\hspace{0.05cm}.$$




'''5.'''  Die Grafik $s_1(t)$ zeigt, dass innerhalb eines Zeitintervalls T entweder 4 oder 8 Schwingungen auftreten:
$$4 \le f_{\rm A}(t) \cdot T \le 8\hspace{0.05cm}.$$
Unter Berücksichtigung der Trägerfrequenz $f_T · T = 6$ ergibt sich für den (normierten) Frequenzhub:
$$\Delta f_{\rm A} \cdot T \hspace{0.15cm}\underline {=2}\hspace{0.05cm}.$$


'''6.'''Der Frequenzhub kann auch wie folgt dargestellt werden:
'''(6)'''&nbsp;  The frequency deviation can also be represented as follows:
$$\Delta f_{\rm A} = \frac {K_{\rm FM}}{2\pi}\cdot A \hspace{0.05cm}.$$
:$$\Delta f_{\rm A} = \frac {K_{\rm FM}}{2\pi}\cdot A \hspace{0.05cm}.$$
Mit $Δf_A · T = 2$ erhält man somit
*With &nbsp; $Δf_{\rm A} · {\rm A}  = 2$&nbsp; we thus get:
$$K_{\rm FM} = \frac {2 \cdot 2\pi}{A \cdot T}= \frac {4\pi}{2\,{\rm V} \cdot 1\,{\rm ms}}\hspace{0.15cm}\underline {= 6283 \,{\rm V}^{-1}{\rm s}^{-1}} \hspace{0.05cm}.$$
:$$K_{\rm FM} = \frac {2 \cdot 2\pi}{A \cdot T}= \frac {4\pi}{2\,{\rm V} \cdot 1\,{\rm ms}}\hspace{0.15cm}\underline {= 6283 \,{\rm V}^{-1}{\rm s}^{-1}} \hspace{0.05cm}.$$


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[[Category:Aufgaben zu Modulationsverfahren|^3.2 Frequenzmodulation (FM)^]]
[[Category:Modulation Methods: Exercises|^3.2 Frequency Modulation^]]
[[de:Aufgaben:Aufgabe 3.5: PM und FM bei Rechtecksignalen]]

Latest revision as of 17:54, 16 March 2026

Two signal waveforms in angle modulation

Assume a bipolar and rectangular source signal $q(t)$ , as shown in the upper diagram.  This signal can only take on the two signal values  $±A = ±2 \ \rm V$  and the duration of the positive and negative rectangles are each $T = 1 \ \rm ms$.  The period of  $q(t)$  is therefore  $T_0 = 2 \ \rm ms$.

The signals $s_1(t)$  and  $s_2(t)$  display two transmitted signals with angle modulation  $\rm (WM)$, each of which can be represented as

$$s(t) = A_{\rm T} \cdot \cos \hspace{-0.05cm}\big [\psi (t) \big ]$$

Here, we distinguish between phase modulation  $\rm (PM)$  with the angular function

$$\psi(t) = \omega_{\rm T} \cdot t + \phi(t) = \omega_{\rm T} \cdot t + K_{\rm PM} \cdot q(t)$$

and frequency modulation  $\rm (FM)$, where the instantaneous freqiency is linearly related to $q(t)$:

$$f_{\rm A}(t) = \frac{\omega_{\rm A}(t)}{2\pi}, \hspace{0.3cm} \omega_{\rm A}(t) = \frac{{\rm d}\hspace{0.03cm}\psi(t)}{{\rm d}t}= \omega_{\rm T} + K_{\rm FM} \cdot q(t)\hspace{0.05cm}.$$

$K_{\rm PM}$  and  $K_{\rm FM}$  denote the dimensionally constrained constants given by the realizations of the PM and FM modulators, respectively.  The frequency deviation  $Δf_{\rm A}$  indicates the maximum deviation of the instantaneous frequency from the carrier frequency.





Hints:

  • In anticipation of the fourth chapter, it should be mentioned that phase modulation with a digital input signal is also called Phase Shift Keying  $\rm (PSK)$  and frequency modulation is analogously called Frequency Shift Keying  $\rm (FSK)$ .


Questions

1 Which of the signals is due to phase modulation and which is due to frquency modulation?

$s_1(t)$  represents a phase modulation.
$s_1(t)$  represents a frequency modulation.

2 What is the carrier phase  $ϕ_{\rm T}$ that could be measured without a message signal   ⇒   $q(t) \equiv 0$ ?

$ϕ_{\rm T} \ = \ $ $\ \rm Grad$

3 What carrier frequency  $($with respect to  $1/T)$  was used in the graphs?

$f_{\rm T} · T \ = \ $

4 The phase of the PM signal is  $±90^\circ$.  What is the modulator constant?

$K_{\rm PM} \ = \ $ $\ \rm V^{-1}$

5 What is the frequency deviation  $Δf_{\rm A}$  of the FM signal with respect to  $1/T$?

$Δf_{\rm A} · T \ = \ $

6 What is the FM modulator constant?

$K_{\rm FM} \ = \ $ $\ \rm (Vs)^{-1}$


Solution

(1)  Answer 2 is correct:

  • For a rectangular (digital) source signal, phase modulation (PM) can be recognised by the typical phase jumps – see the signal waveform  $s_2(t)$.
  • Frequency modulation (FM), on the other hand, has diverse instantaneous frequencies at different times, as in  $s_1(t)$.


(2)  When  $q(t) = 0$ , the equations provided for both PM and FM give

$$s(t) = A_{\rm T} \cdot \cos (\omega_{\rm T} \cdot t ) \hspace{0.3cm}\Rightarrow\hspace{0.3cm} \phi_{\rm T} \hspace{0.15cm}\underline {= 0}\hspace{0.05cm}.$$


(3)  The carrier frequency  $f_{\rm T}$  can be directly determined only from the PM signal   $s_2(t)$ .

  • By counting the oscillations of  $s_2(t)$  in the time interval  $T$ , it can be seen that  $f_{\rm T} · T\hspace{0.15cm}\underline{ = 6}$  was used.
  • When frequency modulating a bipolar source signal,   $f_{\rm T}$  does not occur directly.
  • However, the graphs do indicate that   $f_{\rm T} · T = 6$  is also used here.



(4)  The amplitude value  $A = 2 \ \rm V$  results in the phase  $90^\circ$  or  $π/2$  (minus sine wave).  This gives:

$$K_{\rm PM} = \frac {\pi /2}{2\,{\rm V}} \hspace{0.15cm}\underline {= 0.785\,{\rm V}^{-1}} \hspace{0.05cm}.$$


(5)  The graph for  $s_1(t)$  shows that either four or eight oscillations arise within a time interval  $T$ :   $4 \le f_{\rm A}(t) \cdot T \le 8\hspace{0.05cm}.$

  • Considering the (normalized) carrier frequency  $f_{\rm T} · T = 6$ , the (normalized) frequency deviation is:
$$\Delta f_{\rm A} \cdot T \hspace{0.15cm}\underline {=2}\hspace{0.05cm}.$$


(6)  The frequency deviation can also be represented as follows:

$$\Delta f_{\rm A} = \frac {K_{\rm FM}}{2\pi}\cdot A \hspace{0.05cm}.$$
  • With   $Δf_{\rm A} · {\rm A} = 2$  we thus get:
$$K_{\rm FM} = \frac {2 \cdot 2\pi}{A \cdot T}= \frac {4\pi}{2\,{\rm V} \cdot 1\,{\rm ms}}\hspace{0.15cm}\underline {= 6283 \,{\rm V}^{-1}{\rm s}^{-1}} \hspace{0.05cm}.$$