Difference between revisions of "Aufgaben:Exercise 4.15: MSK Compared with BPSK and QPSK"

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[[File:P_ID1745__Mod_A_4_14.png|right|frame|Leistungsdichtespektren:   BPSK, QPSK, MSK]]
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[[File:EN_Mod_A_4_14_neu.png|right|frame|Power-spectral densities:   BPSK, QPSK, MSK]]
Verglichen werden die Leistungsdichtespektren (im äquivalenten Tiefpassbereich) von
+
Compare the power-spectral densities (in the equivalent low-pass range) of
 
* ''Binary Phase Shift Keying''  $\rm (BPSK)$,
 
* ''Binary Phase Shift Keying''  $\rm (BPSK)$,
 
* ''Quaternary Phase Shift Keying''  $\rm  (QPSK)$,
 
* ''Quaternary Phase Shift Keying''  $\rm  (QPSK)$,
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Diese sind in der Grafik logarithmisch dargestellt, wobei die Frequenz auf den Kehrwert der Bitdauer  $T_{\rm B}$  normiert ist.  
+
These are shown logarithmically in the graph, with frequency normalized to the reciprocal of the bit duration  $T_{\rm B}$ .  
  
  
Für die BPSK und die QPSK ist jeweils ein rechteckförmiger Grundimpuls der Höhe  $s_0$  und der Symboldauer  $T$  vorausgesetzt.  Damit gilt für die BPSK und die QPSK  (bzw. die 4–QAM und die Offset–QPSK)  gleichermaßen:
+
For both BPSK and QPSK, a rectangular fundamental pulse of height  $s_0$  and symbol duration   $T$  is assumed. Thus, for BPSK and QPSK (as well as 4-QAM and offset QPSK), the same applies:
 
:$${\it \Phi}_{s}(f) = \frac{s_0^2 \cdot T}{4} \cdot \big [ {\rm si}^2 ( \pi T \cdot (f- f_{\rm T}) ) + {\rm si}^2 ( \pi T \cdot (f+ f_{\rm T}) ) \big ]\hspace{0.05cm},$$
 
:$${\it \Phi}_{s}(f) = \frac{s_0^2 \cdot T}{4} \cdot \big [ {\rm si}^2 ( \pi T \cdot (f- f_{\rm T}) ) + {\rm si}^2 ( \pi T \cdot (f+ f_{\rm T}) ) \big ]\hspace{0.05cm},$$
und in den äquivalenten Tiefpassbereich transformiert:
+
and transformed into the equivalent low-pass range:
 
:$$ {\it \Phi}_{s,\hspace{0.05cm} {\rm TP}}(f) = \frac{s_0^2 \cdot T}{2} \cdot {\rm si}^2 ( \pi f T ) \hspace{0.05cm}.$$
 
:$$ {\it \Phi}_{s,\hspace{0.05cm} {\rm TP}}(f) = \frac{s_0^2 \cdot T}{2} \cdot {\rm si}^2 ( \pi f T ) \hspace{0.05cm}.$$
  
Trotz gleicher Formel weisen die BPSK und die QPSK unterschiedliche  Leistungsdichtespektren auf:
+
Despite having the same formula, BPSK and QPSK have different power-spectral densities:
*Bei der BPSK  (graue Kurve)  ist die Symboldauer  $T$  gleich der Bitdauer  $T_{\rm B}$  und es gilt mit der Energie pro Bit  $(E_{\rm B} = s_0^2 · T_{\rm B}/2)$ :
+
*In BPSK  (grey curve)  the symbol duration  $T$  is equal to the bit duration  $T_{\rm B}$  with an energy per bit of  $(E_{\rm B} = s_0^2 · T_{\rm B}/2)$ , it holds that:
 
:$${\it \Phi}_{s,\hspace{0.05cm} {\rm TP}}(f) = E_{\rm B} \cdot {\rm si}^2 ( \pi f T_{\rm B} ) \hspace{0.05cm}.$$
 
:$${\it \Phi}_{s,\hspace{0.05cm} {\rm TP}}(f) = E_{\rm B} \cdot {\rm si}^2 ( \pi f T_{\rm B} ) \hspace{0.05cm}.$$
*Dagegen ist bei der QPSK (blaue Kurve) bei gleichem  $E_{\rm B}$  die Symboldauer  $T$  doppelt so groß:
+
*In contrast, in QPSK (blue curve) for the same  $E_{\rm B}$ , the symbol duration  $T$  is doubled:
 
:$${\it \Phi}_{s,\hspace{0.05cm} {\rm TP}}(f) = 2 \cdot E_{\rm B} \cdot {\rm si}^2 ( 2\pi f T_{\rm B} ) \hspace{0.05cm}.$$
 
:$${\it \Phi}_{s,\hspace{0.05cm} {\rm TP}}(f) = 2 \cdot E_{\rm B} \cdot {\rm si}^2 ( 2\pi f T_{\rm B} ) \hspace{0.05cm}.$$
  
  
Bei der Berechnung des MSK–Spektrums (rote Kurve) kann berücksichtigt werden, dass die MSK als Offset–QPSK entsprechend dem  [[Modulationsverfahren/Nichtlineare_Modulationsverfahren#Realisierung_der_MSK_als_Offset.E2.80.93QPSK_.281.29|Blockschaltbild]]  im Theorieteil realisiert werden kann, wenn der folgende Grundimpuls verwendet wird:
+
When calculating the MSK spectrum (red curve), one can take into account that MSK can be realized as an offset QPSK as in the [[Modulation_Methods/Nonlinear_Digital_Modulation#Realizing_MSK_as_Offset.E2.80.93QPSK|block diagram]]  in the theory section if the following fundamental pulse is used:
:$$g(t) = \left\{ \begin{array}{l} g_0 \cdot \cos (\pi/2 \cdot t/T) \\ 0 \\ \end{array} \right.\quad \begin{array}{*{5}c}{\rm{f\ddot{u}r}} \\{\rm{f\ddot{u}r}} \\ \end{array}\begin{array}{*{10}c} -T \le t \le +T \hspace{0.05cm}, \\ {\rm sonst}\hspace{0.05cm}. \\ \end{array}$$
+
:$$g(t) = \left\{ \begin{array}{l} g_0 \cdot \cos (\pi/2 \cdot t/T) \\ 0 \\ \end{array} \right.\quad \begin{array}{*{5}c}{\rm{for}} \\{\rm{otherwise}} \\ \end{array}\begin{array}{*{10}c} -T \le t \le +T \hspace{0.05cm}, \\ {\rm }\hspace{0.05cm}. \\ \end{array}$$
In der  [[Aufgaben:4.15Z_MSK–Grundimpuls_und_MSK-Spektrum|Aufgabe 4.14Z]]  wird die zugehörige Spektralfunktion berechnet:
+
The corresponding spectral function is calculated in  [[Aufgaben:Exercise_4.15Z:_MSK_Basic_Pulse_and_MSK_Spectrum|Exercise 4.15Z]] :
 
:$$G(f) = \frac {4}{\pi}\cdot g_0 \cdot T \cdot \frac{ {\rm cos} ( 2 \pi f T )}{1 - (4 f T)^2 }\hspace{0.05cm}.$$
 
:$$G(f) = \frac {4}{\pi}\cdot g_0 \cdot T \cdot \frac{ {\rm cos} ( 2 \pi f T )}{1 - (4 f T)^2 }\hspace{0.05cm}.$$
  
Berücksichtigen Sie weiterhin:
+
Additionally, consider:
* Die beiden Signale  $s_{\rm I}(t)$  und  $s_{\rm Q}(t)$  sind trotz der Vorcodierung unkorreliert.
+
* The two signals  $s_{\rm I}(t)$  and  $s_{\rm Q}(t)$  are uncorrelated despite prior encoding.
* Bei MSK ist entgegen der QPSK wie bei der BPSK  $T = T_{\rm B}$  zu setzen.
+
* For MSK, contrary to QPSK, one should set  $T = T_{\rm B}$  as in BPSK.
* Auch bei MSK ist die Energie pro Bit wie folgt gegeben:   $E_{\rm B} = s_0^2 · T/2$.
+
* Also, the energy per bit in MSK is given as:   $E_{\rm B} = s_0^2 · T/2$.
* Der Betrag des Tiefpass–Signals  $|s_{\rm TP}(t)| = s_0$  ist gleich dem Maximalwert  $g_0$  des Grundimpulses  $g(t)$.  
+
* The magnitude of the low-pass signal  $|s_{\rm TP}(t)| = s_0$  is equal to the maximum value $g_0$  of the fundamental pulse  $g(t)$.  
  
  
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''Hinweise:''  
+
''Hints:''  
*Die Aufgabe gehört zum  Kapitel  [[Modulationsverfahren/Nichtlineare_digitale_Modulation|Nichtlineare digitale Modulation]].
+
*This exercise belongs to the chapter  [[Modulation_Methods/Nonlinear_Digital_Modulation|Nonlinear Digital Modulation]].
*Bezug genommen wird insbesondere auf den Abschnitt  [[Modulationsverfahren/Nichtlineare_digitale_Modulation#Realisierung_der_MSK_als_Offset.E2.80.93QPSK|Realisierung der MSK als Offset-QPSK]].
+
*Particular reference is made to the section  [[Modulation_Methods/Nonlinear_Digital_Modulation#Realizing_MSK_as_Offset.E2.80.93QPSK|Realizing MSK as Offset–QPSK]].
 
   
 
   
*Das Leistungsdichtespektrums im äquivalenten Tiefpassbereich eines Zweiges zum Beispiel:  Inphasekomponente lautet:
+
*The power-spectral density in the equivalent low-pass range of one branch for example:  the in-phase component is:
 
:$${\it \Phi}_{s,\hspace{0.05cm} {\rm I},\hspace{0.05cm} {\rm TP}}(f) = \frac{1}{2 T} \cdot {\rm E} \left [ a_\nu ^2 \right ] \cdot |G(f)|^2 \hspace{0.05cm}.$$
 
:$${\it \Phi}_{s,\hspace{0.05cm} {\rm I},\hspace{0.05cm} {\rm TP}}(f) = \frac{1}{2 T} \cdot {\rm E} \left [ a_\nu ^2 \right ] \cdot |G(f)|^2 \hspace{0.05cm}.$$
  
  
  
===Fragebogen===
+
===Questions===
  
 
<quiz display=simple>
 
<quiz display=simple>
{Bei welcher Frequenz &nbsp;$f_1$&nbsp; hat das BPSK–Leistungsdichtespektrum seine erste Nullstelle?&nbsp; Der Bezugswert ist die Bitrate &nbsp;$1/T_{\rm B}$.
+
{At what frequency &nbsp;$f_1$&nbsp;does the BPSK power spectral density have its first null point?&nbsp; The reference value is the bitrate &nbsp;$1/T_{\rm B}$.
 
|type="{}"}
 
|type="{}"}
 
$f_1 \ = \ $  { 1 3% } $\ \cdot 1/T_{\rm B}$  
 
$f_1 \ = \ $  { 1 3% } $\ \cdot 1/T_{\rm B}$  
  
{Bei welcher Frequenz &nbsp;$f_1$&nbsp; hat das QPSK–Leistungsdichtespektrum seine erste Nullstelle?
+
{At what frequency &nbsp;$f_1$&nbsp; does the QPSK power-spectral density have its first null point?
 
|type="{}"}
 
|type="{}"}
 
$f_1 \ = \ $ { 0.5 3% } $\ \cdot 1/T_{\rm B}$  
 
$f_1 \ = \ $ { 0.5 3% } $\ \cdot 1/T_{\rm B}$  
  
{Wie lautet das MSK–Leistungsdichtespektrum im äquivalenten TP–Bereich?&nbsp; Welcher LDS–Wert&nbsp; $($normiert auf &nbsp;$E_{\rm B})$&nbsp; tritt bei &nbsp;$f = 0$&nbsp; auf?
+
{What is the MSK power-spectral density in the equivalent low-pass range?&nbsp; What PSD value&nbsp; $($normalized to&nbsp;$E_{\rm B})$&nbsp; occurs at &nbsp;$f = 0$&nbsp;?
 
|type="{}"}
 
|type="{}"}
 
${\itΦ}_\text{s, TP}(f = 0) \ = \ $ { 3.243 3% } $\ \cdot E_{\rm B}$
 
${\itΦ}_\text{s, TP}(f = 0) \ = \ $ { 3.243 3% } $\ \cdot E_{\rm B}$
  
{Welche Aussagen treffen hinsichtlich des asymptotischen Spektralverhaltens zu?
+
{Regarding the asymptotic spectral behaviour, which statements are true?
 
|type="[]"}
 
|type="[]"}
- Die erste LDS–Nullstelle kommt bei MSK früher als bei QPSK.
+
- The first PSD zero comes earlier in MSK than in QPSK.
+ Das MSK–Leistungsdichtespektrum klingt schneller ab im Vergleich zur QPSK.
+
+ The MSK power-spectral density decays faster than that in QPSK.
- Bei MSK ist das Integral über &nbsp;${\itΦ}_\text{s, TP}(f)$&nbsp; (nicht logarithmiert!)&nbsp; größer als bei QPSK.
+
- For MSK, the integral over &nbsp;${\itΦ}_\text{s, TP}(f)$&nbsp; (not logarithmized!)&nbsp; is larger than in QPSK.
  
 
</quiz>
 
</quiz>
  
===Musterlösung===
+
===Solution===
 
{{ML-Kopf}}
 
{{ML-Kopf}}
'''(1)'''&nbsp;  Aus der angegebenen Gleichung und der Grafik erkennt man, dass bei ''Binary Phase Shift Keying'' (BPSK) die erste Nullstelle des Leistungsdichtespektrums bei $f_1\hspace{0.15cm}\underline{ =1} \cdot  1/T_{\rm B}$ liegt.
+
'''(1)'''&nbsp;  From the equation and graph it can be seen that in the case of&nbsp; ''Binary Phase Shift Keying''&nbsp; $\rm (BPSK)$&nbsp;, the first zero of the power-spectral densityis at &nbsp; $f_1\hspace{0.15cm}\underline{ =1} \cdot  1/T_{\rm B}$&nbsp;.
  
  
'''(2)'''&nbsp; Aufgrund der niedrigeren Symbolrate $1/T$ ist bei ''Quaternary Phase Shift Keying'' (QPSK)  &ndash; und bei allen verwandten quaternären Modulationsverfahren &ndash;  das Spektrum nur halb so breit wie bei der BPSK &nbsp; ⇒ &nbsp; $f_1\hspace{0.15cm}\underline{ =0.5} \cdot  1/T_{\rm B}$.
 
  
 +
'''(2)'''&nbsp; Due to the lower symbol rate $1/T$,i&nbsp; ''Quaternary Phase Shift Keying''&nbsp; $\rm (QPSK)$&nbsp;  &ndash; as well as all related quarternary modulation methods &ndash; has a spectrum half as wide as in BPSK &nbsp; ⇒ &nbsp; $f_1\hspace{0.15cm}\underline{ =0.5} \cdot  1/T_{\rm B}$.
  
'''(3)'''&nbsp; Für das Leistungsdichtespektren (LDS) des Gesamtsignals gilt im äquivalenten Tiefpassbereich:
+
 
 +
 
 +
'''(3)'''&nbsp; The power-spectral density &nbsp; $\rm (PSD)$&nbsp; of the total signal in the equivalent low-pass range is given by:
 
:$${\it \Phi}_{s,\hspace{0.05cm} {\rm TP}}(f)  =  {\it \Phi}_{s,\hspace{0.05cm} {\rm I},\hspace{0.05cm} {\rm TP}}(f) + {\it \Phi}_{s,\hspace{0.05cm} {\rm Q},\hspace{0.05cm} {\rm TP}}(f)=  2 \cdot {\it \Phi}_{s,\hspace{0.05cm} {\rm I},\hspace{0.05cm} {\rm TP}}(f) = {1}/{ T} \cdot |G(f)|^2\hspace{0.05cm}.$$
 
:$${\it \Phi}_{s,\hspace{0.05cm} {\rm TP}}(f)  =  {\it \Phi}_{s,\hspace{0.05cm} {\rm I},\hspace{0.05cm} {\rm TP}}(f) + {\it \Phi}_{s,\hspace{0.05cm} {\rm Q},\hspace{0.05cm} {\rm TP}}(f)=  2 \cdot {\it \Phi}_{s,\hspace{0.05cm} {\rm I},\hspace{0.05cm} {\rm TP}}(f) = {1}/{ T} \cdot |G(f)|^2\hspace{0.05cm}.$$
Hierbei ist berücksichtigt, dass
+
This takes into account, that
* die Signale $s_{\rm I}(t)$ und $s_{\rm Q}(t)$ unkorreliert sind, so dass man die LDS–Anteile addieren kann,
+
* the signals&nbsp; $s_{\rm I}(t)$&nbsp; and&nbsp; $s_{\rm Q}(t)$&nbsp; are uncorrelated sind, such that one can add the PSD components,
* wegen der binären bipolaren Amplitudenkoeffizienten der Erwartungswert $E[a_ν^2] = 1$ ist.
+
* and that the expected value is &nbsp; $E[a_ν^2] = 1$&nbsp;, due to the binary bipolar amplitude coefficients.
  
  
Damit erhält man:
+
This gives:
 
:$${\it \Phi}_{s,\hspace{0.05cm} {\rm TP}}(f)= \frac{1}{ T} \cdot \left ( \frac {4}{\pi} \right ) ^2 \cdot g_0^2 \cdot T^2 \cdot \frac{ {\rm cos}^2 ( 2 \pi f T )}{ \big [1 - (4 f T)^2 \big ] ^2} \hspace{0.05cm}.$$
 
:$${\it \Phi}_{s,\hspace{0.05cm} {\rm TP}}(f)= \frac{1}{ T} \cdot \left ( \frac {4}{\pi} \right ) ^2 \cdot g_0^2 \cdot T^2 \cdot \frac{ {\rm cos}^2 ( 2 \pi f T )}{ \big [1 - (4 f T)^2 \big ] ^2} \hspace{0.05cm}.$$
Mit $s_0 = g_0$, $T = T_{\rm B}$ und $E_{\rm B} = s_0^2 · T_{\rm B}/2$ gilt weiter:
+
With&nbsp; $s_0 = g_0$,&nbsp; $T = T_{\rm B}$&nbsp; and&nbsp; $E_{\rm B} = s_0^2 · T_{\rm B}/2$&nbsp;, it further holds that:
 
:$${\it \Phi}_{s,\hspace{0.05cm} {\rm TP}}(f)= \frac{32}{ \pi^2} \cdot E_{\rm B} \cdot \frac{ {\rm cos}^2 ( 2 \pi \cdot f \cdot T_{\rm B} )}{ \big [1 - (4 \cdot f \cdot T_{\rm B})^2 \big ] ^2}\hspace{0.3cm}
 
:$${\it \Phi}_{s,\hspace{0.05cm} {\rm TP}}(f)= \frac{32}{ \pi^2} \cdot E_{\rm B} \cdot \frac{ {\rm cos}^2 ( 2 \pi \cdot f \cdot T_{\rm B} )}{ \big [1 - (4 \cdot f \cdot T_{\rm B})^2 \big ] ^2}\hspace{0.3cm}
 
  \Rightarrow \hspace{0.3cm} {\it \Phi}_{s,\hspace{0.05cm} {\rm TP}}(f = 0 )= \frac{32}{ \pi^2} \cdot E_{\rm B} \hspace{0.15cm}\underline {\approx 3.243 \cdot E_{\rm B}} \hspace{0.05cm}.$$
 
  \Rightarrow \hspace{0.3cm} {\it \Phi}_{s,\hspace{0.05cm} {\rm TP}}(f = 0 )= \frac{32}{ \pi^2} \cdot E_{\rm B} \hspace{0.15cm}\underline {\approx 3.243 \cdot E_{\rm B}} \hspace{0.05cm}.$$
  
'''(4)'''&nbsp; Richtig ist <u>nur der Lösungsvorschlag 1</u>:
+
 
*Bereits aus der Grafik ist zu ersehen, dass die erste Aussage falsch und die zweite richtig ist.  
+
'''(4)'''&nbsp; Only <u>Answer 2</u> is correct:
*Der Lösungsvorschlag 3 stimmt ebenfalls nicht. Das Integral über die Leistungsdichtespektren ergibt die Leistung $(E_{\rm B}/T_{\rm B})$.  
+
*It can already be seen from the graph that the first statement is false and the second is correct.
*Die Signalverläufe von BPSK, QPSK und MSK machen deutlich, dass die Leistung bei konstanter Hüllkurve $(s_0)$ für alle betrachteten Modulationsverfahren gleich ist.
+
(𝐸B/𝑇B).
 +
*Answer 3 is also incorrect. The integral over the power-spectral densities yields the power &nbsp; $(E_{\rm B}/T_{\rm B})$.  
 +
*The signal waveforms of BPSK, QPSK and MSK make it clear that the power with a constant envelope &nbsp; $(s_0)$&nbsp; is the same for these three modulation methods.
  
 
{{ML-Fuß}}
 
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[[Category:Aufgaben zu Modulationsverfahren|^4.4 Nichtlineare digitale Modulation^]]
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[[Category:Modulation Methods: Exercises|^4.4 Non-linear Digital Modulation^]]

Latest revision as of 15:27, 11 April 2022

Power-spectral densities:   BPSK, QPSK, MSK

Compare the power-spectral densities (in the equivalent low-pass range) of

  • Binary Phase Shift Keying  $\rm (BPSK)$,
  • Quaternary Phase Shift Keying  $\rm (QPSK)$,
  • Minimum Shift Keying  $\rm (MSK)$.


These are shown logarithmically in the graph, with frequency normalized to the reciprocal of the bit duration  $T_{\rm B}$ .


For both BPSK and QPSK, a rectangular fundamental pulse of height  $s_0$  and symbol duration  $T$  is assumed. Thus, for BPSK and QPSK (as well as 4-QAM and offset QPSK), the same applies:

$${\it \Phi}_{s}(f) = \frac{s_0^2 \cdot T}{4} \cdot \big [ {\rm si}^2 ( \pi T \cdot (f- f_{\rm T}) ) + {\rm si}^2 ( \pi T \cdot (f+ f_{\rm T}) ) \big ]\hspace{0.05cm},$$

and transformed into the equivalent low-pass range:

$$ {\it \Phi}_{s,\hspace{0.05cm} {\rm TP}}(f) = \frac{s_0^2 \cdot T}{2} \cdot {\rm si}^2 ( \pi f T ) \hspace{0.05cm}.$$

Despite having the same formula, BPSK and QPSK have different power-spectral densities:

  • In BPSK  (grey curve)  the symbol duration  $T$  is equal to the bit duration  $T_{\rm B}$  with an energy per bit of  $(E_{\rm B} = s_0^2 · T_{\rm B}/2)$ , it holds that:
$${\it \Phi}_{s,\hspace{0.05cm} {\rm TP}}(f) = E_{\rm B} \cdot {\rm si}^2 ( \pi f T_{\rm B} ) \hspace{0.05cm}.$$
  • In contrast, in QPSK (blue curve) for the same  $E_{\rm B}$ , the symbol duration  $T$  is doubled:
$${\it \Phi}_{s,\hspace{0.05cm} {\rm TP}}(f) = 2 \cdot E_{\rm B} \cdot {\rm si}^2 ( 2\pi f T_{\rm B} ) \hspace{0.05cm}.$$


When calculating the MSK spectrum (red curve), one can take into account that MSK can be realized as an offset QPSK as in the block diagram  in the theory section if the following fundamental pulse is used:

$$g(t) = \left\{ \begin{array}{l} g_0 \cdot \cos (\pi/2 \cdot t/T) \\ 0 \\ \end{array} \right.\quad \begin{array}{*{5}c}{\rm{for}} \\{\rm{otherwise}} \\ \end{array}\begin{array}{*{10}c} -T \le t \le +T \hspace{0.05cm}, \\ {\rm }\hspace{0.05cm}. \\ \end{array}$$

The corresponding spectral function is calculated in  Exercise 4.15Z :

$$G(f) = \frac {4}{\pi}\cdot g_0 \cdot T \cdot \frac{ {\rm cos} ( 2 \pi f T )}{1 - (4 f T)^2 }\hspace{0.05cm}.$$

Additionally, consider:

  • The two signals  $s_{\rm I}(t)$  and  $s_{\rm Q}(t)$  are uncorrelated despite prior encoding.
  • For MSK, contrary to QPSK, one should set  $T = T_{\rm B}$  as in BPSK.
  • Also, the energy per bit in MSK is given as:   $E_{\rm B} = s_0^2 · T/2$.
  • The magnitude of the low-pass signal  $|s_{\rm TP}(t)| = s_0$  is equal to the maximum value $g_0$  of the fundamental pulse  $g(t)$.





Hints:

  • The power-spectral density in the equivalent low-pass range of one branch – for example:  the in-phase component – is:
$${\it \Phi}_{s,\hspace{0.05cm} {\rm I},\hspace{0.05cm} {\rm TP}}(f) = \frac{1}{2 T} \cdot {\rm E} \left [ a_\nu ^2 \right ] \cdot |G(f)|^2 \hspace{0.05cm}.$$


Questions

1

At what frequency  $f_1$ does the BPSK power spectral density have its first null point?  The reference value is the bitrate  $1/T_{\rm B}$.

$f_1 \ = \ $

$\ \cdot 1/T_{\rm B}$

2

At what frequency  $f_1$  does the QPSK power-spectral density have its first null point?

$f_1 \ = \ $

$\ \cdot 1/T_{\rm B}$

3

What is the MSK power-spectral density in the equivalent low-pass range?  What PSD value  $($normalized to $E_{\rm B})$  occurs at  $f = 0$ ?

${\itΦ}_\text{s, TP}(f = 0) \ = \ $

$\ \cdot E_{\rm B}$

4

Regarding the asymptotic spectral behaviour, which statements are true?

The first PSD zero comes earlier in MSK than in QPSK.
The MSK power-spectral density decays faster than that in QPSK.
For MSK, the integral over  ${\itΦ}_\text{s, TP}(f)$  (not logarithmized!)  is larger than in QPSK.


Solution

(1)  From the equation and graph it can be seen that in the case of  Binary Phase Shift Keying  $\rm (BPSK)$ , the first zero of the power-spectral densityis at   $f_1\hspace{0.15cm}\underline{ =1} \cdot 1/T_{\rm B}$ .


(2)  Due to the lower symbol rate $1/T$,i  Quaternary Phase Shift Keying  $\rm (QPSK)$  – as well as all related quarternary modulation methods – has a spectrum half as wide as in BPSK   ⇒   $f_1\hspace{0.15cm}\underline{ =0.5} \cdot 1/T_{\rm B}$.


(3)  The power-spectral density   $\rm (PSD)$  of the total signal in the equivalent low-pass range is given by:

$${\it \Phi}_{s,\hspace{0.05cm} {\rm TP}}(f) = {\it \Phi}_{s,\hspace{0.05cm} {\rm I},\hspace{0.05cm} {\rm TP}}(f) + {\it \Phi}_{s,\hspace{0.05cm} {\rm Q},\hspace{0.05cm} {\rm TP}}(f)= 2 \cdot {\it \Phi}_{s,\hspace{0.05cm} {\rm I},\hspace{0.05cm} {\rm TP}}(f) = {1}/{ T} \cdot |G(f)|^2\hspace{0.05cm}.$$

This takes into account, that

  • the signals  $s_{\rm I}(t)$  and  $s_{\rm Q}(t)$  are uncorrelated sind, such that one can add the PSD components,
  • and that the expected value is   $E[a_ν^2] = 1$ , due to the binary bipolar amplitude coefficients.


This gives:

$${\it \Phi}_{s,\hspace{0.05cm} {\rm TP}}(f)= \frac{1}{ T} \cdot \left ( \frac {4}{\pi} \right ) ^2 \cdot g_0^2 \cdot T^2 \cdot \frac{ {\rm cos}^2 ( 2 \pi f T )}{ \big [1 - (4 f T)^2 \big ] ^2} \hspace{0.05cm}.$$

With  $s_0 = g_0$,  $T = T_{\rm B}$  and  $E_{\rm B} = s_0^2 · T_{\rm B}/2$ , it further holds that:

$${\it \Phi}_{s,\hspace{0.05cm} {\rm TP}}(f)= \frac{32}{ \pi^2} \cdot E_{\rm B} \cdot \frac{ {\rm cos}^2 ( 2 \pi \cdot f \cdot T_{\rm B} )}{ \big [1 - (4 \cdot f \cdot T_{\rm B})^2 \big ] ^2}\hspace{0.3cm} \Rightarrow \hspace{0.3cm} {\it \Phi}_{s,\hspace{0.05cm} {\rm TP}}(f = 0 )= \frac{32}{ \pi^2} \cdot E_{\rm B} \hspace{0.15cm}\underline {\approx 3.243 \cdot E_{\rm B}} \hspace{0.05cm}.$$


(4)  Only Answer 2 is correct:

  • It can already be seen from the graph that the first statement is false and the second is correct.

(𝐸B/𝑇B).

  • Answer 3 is also incorrect. The integral over the power-spectral densities yields the power   $(E_{\rm B}/T_{\rm B})$.
  • The signal waveforms of BPSK, QPSK and MSK make it clear that the power with a constant envelope   $(s_0)$  is the same for these three modulation methods.