Difference between revisions of "Aufgaben:Exercise 3.1: Phase Modulation Locus Curve"

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{{quiz-Header|Buchseite=Modulationsverfahren/Phasenmodulation (PM)
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{{quiz-Header|Buchseite=Modulation_Methods/Phase_Modulation_(PM)
 
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<quiz display=simple>
 
<quiz display=simple>
{Which modulation method is used in modulator &nbsp;$\rm M_1$?
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{Which modulation method is used by modulator &nbsp;$\rm M_1$?
 
|type="()"}
 
|type="()"}
 
- Double-sideband amplitude modulation.
 
- Double-sideband amplitude modulation.
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- Phase modulation.
 
- Phase modulation.
  
{Welches Modulationsverfahren verwendet der Modulator &nbsp;$\rm M_2$?
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{Which modulation method is used by modulator &nbsp;$\rm M_2$?
 
|type="()"}
 
|type="()"}
- Zweiseitenband–Amplitudenmodulation.
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- Double-sideband amplitude modulation.
- Einseitenband–Amplitudenmodulation.
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- Single sideband amplitude modulation.
+ Phasenmodulation.
+
+ Phase modulation.
  
{Wie groß ist die Trägeramplitude &nbsp;$A_{\rm T}$&nbsp; beim Phasenmodulator?&nbsp; Beachten Sie die Normierung auf &nbsp;$1 \ \rm V$.
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{What is the carrier amplitude &nbsp;$A_{\rm T}$&nbsp; for the phase modulator?&nbsp; Note the normalization to &nbsp;$1 \ \rm V$.
 
|type="{}"}
 
|type="{}"}
 
$A_{\rm T} \ = \ $ { 1 3% } $\ \rm V$  
 
$A_{\rm T} \ = \ $ { 1 3% } $\ \rm V$  
  
{Welche Werte besitzen der Modulationsindex &nbsp;$η$&nbsp; und die Modulatorkonstante &nbsp;$K_{\rm PM}$?
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{What are the values of the modulation index &nbsp;$η$&nbsp; and the modulator constant &nbsp;$K_{\rm PM}$?
 
|type="{}"}
 
|type="{}"}
 
$η\ = \ $  { 3.1415 3% }  
 
$η\ = \ $  { 3.1415 3% }  
 
$K_{\rm PM}\ = \ $ { 1.571 3% } $\ \rm 1/V$
 
$K_{\rm PM}\ = \ $ { 1.571 3% } $\ \rm 1/V$
  
{Beschreiben Sie die Bewegung auf der Ortskurve.&nbsp; Zu welcher Zeit &nbsp;$t_1$&nbsp; wird erstmals wieder der Ausgangspunkt &nbsp;$s_{\rm TP}(t = 0) = -1 \ \rm V$&nbsp; erreicht?
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{Describe the motion on the locus curve. At what time&nbsp;$t_1$&nbsp; is the starting point &nbsp;$s_{\rm TP}(t = 0) = -1 \ \rm V$&nbsp; first reached again?
 
|type="{}"}
 
|type="{}"}
 
$t_1\ = \ $ { 100 3% } $ \ \rm  &micro; s$
 
$t_1\ = \ $ { 100 3% } $ \ \rm  &micro; s$
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</quiz>
 
</quiz>
  
===Musterlösung===
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===Solution===
 
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'''(1)'''&nbsp; Es handelt sich um eine ESB–AM mit dem Seitenband–zu–Träger–Verhältnis&nbsp; $μ = 1$ &nbsp; ⇒ &nbsp; <u>Antwort 2</u>:
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'''(1)'''&nbsp; We are dealing with SSB-AM with a sideband-to-carrier ratio $μ = 1$ &nbsp; ⇒ &nbsp; <u>Answer 2</u>:
*Bewegt man sich auf dem Kreis in mathematisch positive Richtung, so liegt speziell eine OSB–AM vor, andernfalls eine USB–AM.
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*If one moves in the mathematically positive direction on the circle, it is specifically an USB–AM, otherwise it is a LSB–AM.
*Die Phasenfunktion&nbsp; $ϕ(t)$&nbsp; als der Winkel eines Punktes&nbsp; $s_{\rm TP}(t)$&nbsp; auf dem Kreis(bogen) bezogen auf den Koordinatenursprung kann Werte zwischen&nbsp; $±π/2$&nbsp; annehmen und zeigt keinen Cosinusverlauf.  
+
*The phase function&nbsp; $ϕ(t)$&nbsp; as the angle of a point&nbsp; $s_{\rm TP}(t)$&nbsp; on the circle (arc) with respect to the coordinate origin can take values between&nbsp; $±π/2$&nbsp; and does not show a cosine progression.  
*Aber auch die Hüllkurve&nbsp; $a(t) = |s_{\rm TP}(t)|$&nbsp; ist nicht cosinusförmig.  
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*The envelope &nbsp; $a(t) = |s_{\rm TP}(t)|$&nbsp; is also not cosine.  
*Würde man beim Empfänger für&nbsp; $\rm M_1$&nbsp; einen Hüllkurvendemodulator einsetzen, so käme es zu nichtlinearen Verzerrungen im Gegensatz zur ZSB–AM, deren Ortskurve eine horizontale Gerade ist.
+
*If an envelope demodulator were used for&nbsp; $\rm M_1$&nbsp; at the receiver, nonlinear distortions would occur, in contrast to DSB–AM, which has a horizontal straight line for a locus curve.
  
  
  
  
'''(2)'''&nbsp; Hier handelt es sich um die Phasenmodulation &nbsp; ⇒ &nbsp; <u>Antwort 3</u>:
+
'''(2)'''&nbsp; Here, we observe phase modulation &nbsp; ⇒ &nbsp; <u>Answer 3</u>:
*Die Einhüllende&nbsp; $a(t) = A_{\rm T}$&nbsp; ist konstant,  
+
*The envelope &nbsp; $a(t) = A_{\rm T}$&nbsp; is constant,  
*während die Phase&nbsp; $ϕ(t)$&nbsp; entsprechend dem Quellensignal&nbsp; $q(t)$&nbsp; cosinusförmig verläuft.
+
*while the phase&nbsp; $ϕ(t)$&nbsp; is cosinusoidal according to the source signal&nbsp; $q(t)$&nbsp;.
  
  
  
  
'''(3)'''&nbsp; Bei der Phasenmodulation gilt:
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'''(3)'''&nbsp; In the case of phase modulation:
 
:$$s_{\rm TP}(t) = A_{\rm T} \cdot {\rm e}^{\hspace{0.05cm}{\rm j} \hspace{0.05cm}\cdot \hspace{0.05cm}\phi(t) }\hspace{0.05cm}.$$
 
:$$s_{\rm TP}(t) = A_{\rm T} \cdot {\rm e}^{\hspace{0.05cm}{\rm j} \hspace{0.05cm}\cdot \hspace{0.05cm}\phi(t) }\hspace{0.05cm}.$$
*Aus der Grafik kann man die Trägeramplitude&nbsp; $A_{\rm T}\hspace{0.15cm}\underline{ = 1 \ \rm V}$&nbsp; als den Kreisradius ablesen.
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*From the graph, we can read the carrier amplitude &nbsp; $A_{\rm T}\hspace{0.15cm}\underline{ = 1 \ \rm V}$&nbsp; as the radius of the circle.
  
  
  
  
'''(4)'''&nbsp; Das Quellensignal&nbsp; $q(t)$&nbsp; ist zum Zeitpunkt&nbsp; $t = 0$&nbsp; maximal und damit auch die Phasenfunktion:
+
'''(4)'''&nbsp; The source signal&nbsp; $q(t)$&nbsp; is at its maximum at time&nbsp; $t = 0$&nbsp; and therefore so is the phase function:
 
:$$ \eta = \phi_{\rm max} = \phi( t =0) = \pi\hspace{0.15cm}\underline { = 3.1415} \hspace{0.05cm}.$$
 
:$$ \eta = \phi_{\rm max} = \phi( t =0) = \pi\hspace{0.15cm}\underline { = 3.1415} \hspace{0.05cm}.$$
*Daraus erhält man für die Modulatorkonstante:
+
*This gives the modulator constant:
 
$$K_{\rm PM} = \frac{\eta}{A_{\rm N}} = \frac{\pi}{2\,{\rm V}}\hspace{0.15cm}\underline {= 1.571\,{\rm V}^{-1}}\hspace{0.05cm}.$$
 
$$K_{\rm PM} = \frac{\eta}{A_{\rm N}} = \frac{\pi}{2\,{\rm V}}\hspace{0.15cm}\underline {= 1.571\,{\rm V}^{-1}}\hspace{0.05cm}.$$
  
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'''(5)'''&nbsp; Man bewegt sich auf dem Kreis(bogen) im Uhrzeigersinn.  
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'''(5)'''&nbsp; One moves clockwise along the circular arc.  
*Nach einem Viertel der Periodendauer &nbsp;$T_{\rm N} = 1/f_{\rm N}  = 200 \ \rm &micro; s$&nbsp; ist &nbsp;$ϕ(t) = 0$&nbsp; und &nbsp;$s_{\rm TP}(t) = 1 \, \rm V$.  
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*After a quarter of the period &nbsp;$T_{\rm N} = 1/f_{\rm N}  = 200 \ \rm &micro; s$&nbsp;, &nbsp;$ϕ(t) = 0$&nbsp; and &nbsp;$s_{\rm TP}(t) = 1 \, \rm V$.  
*Zur Zeit &nbsp;$t_1 = T_{\rm N}/2\hspace{0.15cm}\underline { = 100 \ \rm &micro; s}$&nbsp; gilt &nbsp;$ϕ(t_1) = -π$&nbsp; und &nbsp;$s_{\rm TP}(t_1) = -1 \, \rm V$.  
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*At time &nbsp;$t_1 = T_{\rm N}/2\hspace{0.15cm}\underline { = 100 \ \rm &micro; s}$&nbsp;, &nbsp;$ϕ(t_1) = -π$&nbsp; and &nbsp;$s_{\rm TP}(t_1) = -1 \, \rm V$.  
*Danach bewegt man sich auf dem Kreisbogen entgegen dem Uhrzeigersinn.
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*Afterwards, one moves counterclockwise along the arc.
  
 
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Latest revision as of 15:54, 9 April 2022

Two locus curves to choose from

The locus curve is generally understood as the plot of the equivalent low-pass signal $s_{\rm TP}(t)$  in the complex plane.

  • The graph shows locus curves at the output of two modulators  $\rm M_1$  and  $\rm M_2$.
  • The real and imaginary parts are each normalized to $1 \ \rm V$ in this graph.


Let the source signal be the same for both modulators: $$ q(t) = A_{\rm N} \cdot \cos(2 \pi f_{\rm N} \cdot t),\hspace{1cm} {\rm with}\hspace{0.2cm} A_{\rm N} = 2\,{\rm V},\hspace{0.2cm}f_{\rm N} = 5\,{\rm kHz}\hspace{0.05cm}.$$ One of the two modulators implements phase modulation, which is characterized by the following equations:

$$ s(t) = A_{\rm T} \cdot \cos \hspace{-0.1cm} \big[\omega_{\rm T} \cdot t + \phi(t) \big]\hspace{0.05cm},$$
$$ s_{\rm TP}(t) = A_{\rm T} \cdot {\rm e}^{\hspace{0.05cm}{\rm j} \hspace{0.05cm}\cdot \hspace{0.05cm}\phi(t) }\hspace{0.05cm},$$
$$ \phi(t) = K_{\rm PM} \cdot q(t)\hspace{0.05cm}.$$

The maximum value  $ϕ(t)$  is called the   modulation index  $η$.  Often  $η$  is also called   phase deviation  in the literature.





Hints:


Questions

1

Which modulation method is used by modulator  $\rm M_1$?

Double-sideband amplitude modulation.
Single sideband amplitude modulation.
Phase modulation.

2

Which modulation method is used by modulator  $\rm M_2$?

Double-sideband amplitude modulation.
Single sideband amplitude modulation.
Phase modulation.

3

What is the carrier amplitude  $A_{\rm T}$  for the phase modulator?  Note the normalization to  $1 \ \rm V$.

$A_{\rm T} \ = \ $

$\ \rm V$

4

What are the values of the modulation index  $η$  and the modulator constant  $K_{\rm PM}$?

$η\ = \ $

$K_{\rm PM}\ = \ $

$\ \rm 1/V$

5

Describe the motion on the locus curve. At what time $t_1$  is the starting point  $s_{\rm TP}(t = 0) = -1 \ \rm V$  first reached again?

$t_1\ = \ $

$ \ \rm µ s$


Solution

(1)  We are dealing with SSB-AM with a sideband-to-carrier ratio $μ = 1$   ⇒   Answer 2:

  • If one moves in the mathematically positive direction on the circle, it is specifically an USB–AM, otherwise it is a LSB–AM.
  • The phase function  $ϕ(t)$  as the angle of a point  $s_{\rm TP}(t)$  on the circle (arc) with respect to the coordinate origin can take values between  $±π/2$  and does not show a cosine progression.
  • The envelope   $a(t) = |s_{\rm TP}(t)|$  is also not cosine.
  • If an envelope demodulator were used for  $\rm M_1$  at the receiver, nonlinear distortions would occur, in contrast to DSB–AM, which has a horizontal straight line for a locus curve.



(2)  Here, we observe phase modulation   ⇒   Answer 3:

  • The envelope   $a(t) = A_{\rm T}$  is constant,
  • while the phase  $ϕ(t)$  is cosinusoidal according to the source signal  $q(t)$ .



(3)  In the case of phase modulation:

$$s_{\rm TP}(t) = A_{\rm T} \cdot {\rm e}^{\hspace{0.05cm}{\rm j} \hspace{0.05cm}\cdot \hspace{0.05cm}\phi(t) }\hspace{0.05cm}.$$
  • From the graph, we can read the carrier amplitude   $A_{\rm T}\hspace{0.15cm}\underline{ = 1 \ \rm V}$  as the radius of the circle.



(4)  The source signal  $q(t)$  is at its maximum at time  $t = 0$  and therefore so is the phase function:

$$ \eta = \phi_{\rm max} = \phi( t =0) = \pi\hspace{0.15cm}\underline { = 3.1415} \hspace{0.05cm}.$$
  • This gives the modulator constant:

$$K_{\rm PM} = \frac{\eta}{A_{\rm N}} = \frac{\pi}{2\,{\rm V}}\hspace{0.15cm}\underline {= 1.571\,{\rm V}^{-1}}\hspace{0.05cm}.$$



(5)  One moves clockwise along the circular arc.

  • After a quarter of the period  $T_{\rm N} = 1/f_{\rm N} = 200 \ \rm µ s$ ,  $ϕ(t) = 0$  and  $s_{\rm TP}(t) = 1 \, \rm V$.
  • At time  $t_1 = T_{\rm N}/2\hspace{0.15cm}\underline { = 100 \ \rm µ s}$ ,  $ϕ(t_1) = -π$  and  $s_{\rm TP}(t_1) = -1 \, \rm V$.
  • Afterwards, one moves counterclockwise along the arc.