Aufgaben:Exercise 1.6Z: Two Optimal Systems: Difference between revisions

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[[File:P_ID1293__Dig_Z_1_6.png|right|frame|Optimal systems in the <br>time and frequency domain]]
[[File:P_ID1293__Dig_Z_1_6.png|right|frame|Optimal systems in time and frequency domain]]
Consider two binary transmission systems &nbsp;$\rm A$&nbsp; and &nbsp;$\rm B$&nbsp;, which have the same error behavior for an AWGN channel with noise power density &nbsp;$N_{0}$.&nbsp; In both cases, the bit error probability is:
Consider two binary transmission systems &nbsp;$\rm A$&nbsp; and &nbsp;$\rm B$,&nbsp; which have the same error behavior for an AWGN channel with noise power density &nbsp;$N_{0}$.&nbsp; In both cases,&nbsp; the bit error probability is:
:$$p_{\rm B} =  {\rm Q} \left( \sqrt{{2 \cdot E_{\rm B}}/{N_0}}\right)\hspace{0.05cm}.$$
:$$p_{\rm B} =  {\rm Q} \left( \sqrt{{2 \cdot E_{\rm B}}/{N_0}}\right)\hspace{0.05cm}.$$
*System &nbsp;$\rm A$&nbsp; uses the NRZ basic transmission pulse &nbsp;$g_{s}(t)$&nbsp; according to the upper sketch with amplitude &nbsp;$s_{0} = 1 \ \rm V$&nbsp; and duration &nbsp;$T = 0.5\ \rm &micro; s$.  
*System &nbsp;$\rm A$&nbsp; uses the NRZ basic transmission pulse &nbsp;$g_{s}(t)$&nbsp; according to the upper sketch with amplitude &nbsp;$s_{0} = 1 \ \rm V$&nbsp; and duration &nbsp;$T = 0.5\ \rm &micro; s$.  
*In contrast, system &nbsp;$\rm B$&nbsp;, which is to operate at the same bit rate as system &nbsp;$\rm A$,&nbsp; has a rectangular basic transmission pulse spectrum:
*In contrast,&nbsp; system &nbsp;$\rm B$,&nbsp; which is to operate at the same bit rate as system &nbsp;$\rm A$,&nbsp; has a rectangular basic transmission pulse spectrum:
:$$G_s(f)  =  \left\{ \begin{array}{c} G_0  \\
:$$G_s(f)  =  \left\{ \begin{array}{c} G_0  \\0 \\  \end{array} \right.\quad\begin{array}{*{1}c} {\rm{for}}\\  {\rm{for}} \\ \end{array}\begin{array}{*{20}c}|f| < f_0 \hspace{0.05cm}, \\|f| > f_0 \hspace{0.05cm}.\\\end{array}$$
0 \\  \end{array} \right.\quad
\begin{array}{*{1}c} {\rm{for}}
\\  {\rm{for}} \\ \end{array}\begin{array}{*{20}c}
|f| < f_0 \hspace{0.05cm}, \\
|f| > f_0 \hspace{0.05cm}.\\
\end{array}$$




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Notes:  
''Notes:''
*The exercise belongs to the chapter&nbsp;  [[Digital_Signal_Transmission/Optimization_of_Baseband_Transmission_Systems|"Optimization of Baseband Transmission Systems"]].
*The exercise belongs to the chapter&nbsp;  [[Digital_Signal_Transmission/Optimization_of_Baseband_Transmission_Systems|Optimization of Baseband Transmission Systems]].
   
   
*Note that here the pulse amplitude is given in "volts", so that the average energy per bit &nbsp;$(E_{\rm B})$&nbsp; has the unit &nbsp;$\rm V^{2}/Hz$.&nbsp;
*Here,&nbsp; the pulse amplitude is given in&nbsp; "volts",&nbsp; so that the average energy per bit &nbsp;$(E_{\rm B})$&nbsp; has the unit &nbsp;$\rm V^{2}/Hz$.&nbsp;




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{Which statements are true for the receiver filters of systems &nbsp;$\rm A$&nbsp; and &nbsp;$\rm B$?
{Which statements are true for the receiver filters of systems &nbsp;$\rm A$&nbsp; and &nbsp;$\rm B$?
|type="[]"}
|type="[]"}
+For system &nbsp;$\rm A$,&nbsp; &nbsp;$H_{\rm E}(f)$&nbsp; has a si-shaped curve.
+For system &nbsp;$\rm A$,&nbsp; &nbsp;$H_{\rm E}(f)$&nbsp; has a sinc-shaped curve.
+For system &nbsp;$\rm B$,&nbsp; &nbsp;$H_{\rm E}(f)$&nbsp; is an ideal rectangular lowpass filter.
+For system &nbsp;$\rm B$,&nbsp; &nbsp;$H_{\rm E}(f)$&nbsp; is an ideal rectangular low-pass filter.
-$H_{\rm E}(f)$&nbsp; can be realized by an integrator in system &nbsp;$\rm B$.&nbsp;  
-$H_{\rm E}(f)$&nbsp; can be realized by an integrator in system &nbsp;$\rm B$.&nbsp;  


{For which cutoff frequency &nbsp;$f_{0}$&nbsp; does system &nbsp;$\rm B$&nbsp; have symbol duration &nbsp;$T$?&nbsp;  
{For which cutoff frequency &nbsp;$f_{0}$&nbsp; does system &nbsp;$\rm B$&nbsp; have the symbol duration &nbsp;$T$?&nbsp;  
|type="{}"}
|type="{}"}
$f_{0} \ = \ ${ 1 3% } $\ \rm MHz$
$f_{0} \ = \ ${ 1 3% } $\ \rm MHz$


{How large should the constant height &nbsp;$G_{0}$&nbsp; of the spectrum of &nbsp;$\rm B$&nbsp; be chosen so that the same energy per bit results as for system &nbsp;$\rm A$?
{How large should the constant height &nbsp;$G_{0}$&nbsp; of the spectrum &nbsp;$\rm B$&nbsp; be chosen so that the same energy per bit results as for system &nbsp; $\rm A$?
|type="{}"}
|type="{}"}
$G_{0} \ = \ $ { 0.5 3% } $\ \cdot 10^{-6} \ \rm V/Hz$
$G_{0} \ = \ $ { 0.5 3% } $\ \cdot 10^{-6} \ \rm V/Hz$
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'''(1)'''&nbsp; Both systems operate according to the specification with the same bit rate.  
'''(1)'''&nbsp; Both systems operate according to the specification with the same bit rate.  
*The NRZ basic transmission pulse of system '''A''' has the symbol duration $T = 0.5\ \rm &micro; s$.  
*The NRZ basic transmission pulse of system&nbsp; $\rm A$&nbsp; has the symbol duration $T = 0.5\ \rm &micro; s$.  
*This results in the bit rate $R = 1/T$ $ \underline{= 2\ \rm Mbit/s}$.
*This results in the bit rate&nbsp; $R = 1/T$ $ \underline{= 2\ \rm Mbit/s}$.




'''(2)'''&nbsp; The energy of the NRZ basic transmission pulse of system '''A''' is given by
'''(2)'''&nbsp; The energy of the NRZ basic transmission pulse of system&nbsp; $\rm A$&nbsp; is given by
:$$E_{\rm B} =
:$$E_{\rm B} =\int_{-\infty}^{+\infty}g_s^2 (t)\,{\rm d} t  =s_0^2 \cdot T =  {1\,{\rm V^2}}\cdot {0.5 \cdot 10^{-6}\,{\rm s}}\hspace{0.1cm}\underline { = 0.5 \cdot 10^{-6}\,{\rm V^2/Hz}}\hspace{0.05cm}.$$
\int_{-\infty}^{+\infty}g_s^2 (t)\,{\rm d} t  =
s_0^2 \cdot T =  {1\,{\rm V^2}}\cdot {0.5 \cdot 10^{-6}\,{\rm s}}\hspace{0.1cm}\underline { = 0.5 \cdot 10^{-6}\,{\rm V^2/Hz}}\hspace{0.05cm}.$$




'''(3)'''&nbsp; The <u>first two statements are true</u>:  
'''(3)'''&nbsp; The&nbsp; <u>first two statements are true</u>:  
*In both cases $h_{\rm E}(t)$ must be equal in form to $g_{s}(t)$ and $H_{\rm E}(f)$ must be equal in form to $G_{s}(f)$.  
*In both cases&nbsp; $h_{\rm E}(t)$&nbsp; must be equal in form to&nbsp; $g_{s}(t)$&nbsp; and&nbsp; $H_{\rm E}(f)$&nbsp; must be equal in form to&nbsp; $G_{s}(f)$.  
*Thus, for system '''A''', the impulse response $h_{\rm E}(t)$ is rectangular and the frequency response $H_{\rm E}(f)$ is si-shaped.  
*Thus, for system&nbsp; $\rm A$,&nbsp; the impulse response&nbsp; $h_{\rm E}(t)$&nbsp; is rectangular and the frequency response&nbsp; $H_{\rm E}(f)$&nbsp; is sinc-shaped.  
*For system '''B''', $H_{\rm E}(f)$ is rectangular like $G_{s}(f)$ and thus the impulse response $h_{\rm E}(t)$ is an si-function.
*For system&nbsp; $\rm B$,&nbsp; $H_{\rm E}(f)$&nbsp; is rectangular like&nbsp; $G_{s}(f)$&nbsp; and thus the impulse response&nbsp; $h_{\rm E}(t)$&nbsp; is an sinc-function.
*Statement 3 is false: &nbsp;  An integrator has a rectangular impulse response and would be suitable for the realization of system '''A''', but not for system '''B'''.
*Statement 3 is false: &nbsp;  An integrator has a rectangular impulse response and would be suitable for the realization of system&nbsp; $\rm A$,&nbsp; but not for system&nbsp; $\rm B$.




'''(4)'''&nbsp; For system '''B''' $G_{d}(f)$ nearly coincides with $G_{s}(f)$.  
'''(4)'''&nbsp; For system&nbsp; $\rm B$ &nbsp; &rArr; &nbsp; $G_{d}(f)$&nbsp; nearly coincides with&nbsp; $G_{s}(f)$.  
*There is only a difference in the Nyquist frequency, but this does not affect the considerations here:
*There is only a difference in the Nyquist frequency,&nbsp; but this does not affect the considerations here:
*While $G_{s}(f_{\rm Nyq}) = 1/2$, $G_{d}(f_{\rm Nyq}) = 1/4$.
*While&nbsp; $G_{s}(f_{\rm Nyq}) = 1/2$,&nbsp; $G_{d}(f_{\rm Nyq}) = 1/4$.


*This results in a Nyquist system with rolloff factor $r = 0$.  
*This results in a Nyquist system with rolloff factor&nbsp; $r = 0$.  
*From this follows for the Nyquist frequency from the condition that the symbol duration should also be $T = 0.5\ \rm &micro; s$:
*From this follows for the Nyquist frequency from the condition that the symbol duration should also be&nbsp; $T = 0.5\ \rm &micro; s$:
:$$f_{\rm 0} = f_{\rm Nyq} = \frac{1 } {2 \cdot T} = \frac{1 } {2 \cdot 0.5 \cdot 10^{-6}\,{\rm s}}\hspace{0.1cm}\underline {= 1\,{\rm MHz}}\hspace{0.05cm}.$$
:$$f_{\rm 0} = f_{\rm Nyq} = \frac{1 } {2 \cdot T} = \frac{1 } {2 \cdot 0.5 \cdot 10^{-6}\,{\rm s}}\hspace{0.1cm}\underline {= 1\,{\rm MHz}}\hspace{0.05cm}.$$
   
   
 
 
'''(5)'''&nbsp; For the energy of the basic transmission pulse can also be written:
'''(5)'''&nbsp; For the energy of the basic transmission pulse can also be written:
:$$E_{\rm B} =
:$$E_{\rm B} =\int_{-\infty}^{+\infty}|G_s(f)|^2 \,{\rm d} f  = G_0^2\cdot 2 f_0\hspace{0.05cm}.$$
\int_{-\infty}^{+\infty}|G_s(f)|^2 \,{\rm d} f  = G_0^2
*Using the results from&nbsp; '''(2)'''&nbsp; and&nbsp; '''(4)''',&nbsp; it follows:
\cdot 2 f_0\hspace{0.05cm}.$$
:$$G_0^2 = \frac{E_{\rm B}}{2 f_0} = \frac{5 \cdot 10^{-7}\,{\rm V^2/Hz}}{2 \cdot 10^{6}\,{\rm Hz}}= 2.5 \cdot 10^{-13}\,{\rm V^2/Hz^2}\hspace{0.3cm}\Rightarrow \hspace{0.3cm}G_0 \hspace{0.1cm}\underline {= 0.5 \cdot 10^{-6}\,{\rm V/Hz}}\hspace{0.05cm}.$$
*Using the results from '''(2)''' and '''(4)''', it follows:
:$$G_0^2 = \frac{E_{\rm B}}{2 f_0} = \frac{5 \cdot 10^{-7}\,{\rm V^2/Hz}}{2 \cdot 10^{6}\,{\rm
Hz}}= 2.5 \cdot 10^{-13}\,{\rm V^2/Hz^2}
\hspace{0.3cm}\Rightarrow \hspace{0.3cm}G_0 \hspace{0.1cm}\underline {= 0.5 \cdot 10^{-6}\,{\rm V/Hz}}
\hspace{0.05cm}.$$




'''(6)'''&nbsp; <u>Solution 1</u> is correct:
'''(6)'''&nbsp; <u>Solution 1</u>&nbsp; is correct:
*System '''A''' represents the optimal system even with peak limitation.
*System&nbsp; $\rm A$&nbsp; represents the optimal system even with peak limitation.
*On the other hand, system '''B''' would be unsuitable due to the extremely unfavorable crest factor.
*On the other hand,&nbsp; system&nbsp; $\rm B$&nbsp; would be unsuitable due to the extremely unfavorable crest factor.


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[[Category:Digital Signal Transmission: Exercises|^1.4 Optimization of Baseband Systems^]]
[[Category:Digital Signal Transmission: Exercises|^1.4 Optimization of Baseband Systems^]]
[[de:Aufgaben:Aufgabe 1.6Z: Zwei Optimalsysteme]]

Latest revision as of 17:54, 16 March 2026


Optimal systems in time and frequency domain

Consider two binary transmission systems  $\rm A$  and  $\rm B$,  which have the same error behavior for an AWGN channel with noise power density  $N_{0}$.  In both cases,  the bit error probability is:

$$p_{\rm B} = {\rm Q} \left( \sqrt{{2 \cdot E_{\rm B}}/{N_0}}\right)\hspace{0.05cm}.$$
  • System  $\rm A$  uses the NRZ basic transmission pulse  $g_{s}(t)$  according to the upper sketch with amplitude  $s_{0} = 1 \ \rm V$  and duration  $T = 0.5\ \rm µ s$.
  • In contrast,  system  $\rm B$,  which is to operate at the same bit rate as system  $\rm A$,  has a rectangular basic transmission pulse spectrum:
$$G_s(f) = \left\{ \begin{array}{c} G_0 \\0 \\ \end{array} \right.\quad\begin{array}{*{1}c} {\rm{for}}\\ {\rm{for}} \\ \end{array}\begin{array}{*{20}c}|f| < f_0 \hspace{0.05cm}, \\|f| > f_0 \hspace{0.05cm}.\\\end{array}$$



Notes:

  • Here,  the pulse amplitude is given in  "volts",  so that the average energy per bit  $(E_{\rm B})$  has the unit  $\rm V^{2}/Hz$. 


Questions

1 At what bit rate do the two systems operate?

$R \ = \ $ $\ \rm Mbit/s$

2 Calculate the energy per bit for system  $\rm A$.

$E_{\rm B} \ = \ $ $\ \cdot 10^{-6} \ \rm V^{2}/Hz$

3 Which statements are true for the receiver filters of systems  $\rm A$  and  $\rm B$?

For system  $\rm A$,   $H_{\rm E}(f)$  has a sinc-shaped curve.
For system  $\rm B$,   $H_{\rm E}(f)$  is an ideal rectangular low-pass filter.
$H_{\rm E}(f)$  can be realized by an integrator in system  $\rm B$. 

4 For which cutoff frequency  $f_{0}$  does system  $\rm B$  have the symbol duration  $T$? 

$f_{0} \ = \ $ $\ \rm MHz$

5 How large should the constant height  $G_{0}$  of the spectrum  $\rm B$  be chosen so that the same energy per bit results as for system   $\rm A$?

$G_{0} \ = \ $ $\ \cdot 10^{-6} \ \rm V/Hz$

6 Would one of the two systems be suitable even with peak limitation?

System  $\rm A$,
System  $\rm B$.


Solution

(1)  Both systems operate according to the specification with the same bit rate.

  • The NRZ basic transmission pulse of system  $\rm A$  has the symbol duration $T = 0.5\ \rm µ s$.
  • This results in the bit rate  $R = 1/T$ $ \underline{= 2\ \rm Mbit/s}$.


(2)  The energy of the NRZ basic transmission pulse of system  $\rm A$  is given by

$$E_{\rm B} =\int_{-\infty}^{+\infty}g_s^2 (t)\,{\rm d} t =s_0^2 \cdot T = {1\,{\rm V^2}}\cdot {0.5 \cdot 10^{-6}\,{\rm s}}\hspace{0.1cm}\underline { = 0.5 \cdot 10^{-6}\,{\rm V^2/Hz}}\hspace{0.05cm}.$$


(3)  The  first two statements are true:

  • In both cases  $h_{\rm E}(t)$  must be equal in form to  $g_{s}(t)$  and  $H_{\rm E}(f)$  must be equal in form to  $G_{s}(f)$.
  • Thus, for system  $\rm A$,  the impulse response  $h_{\rm E}(t)$  is rectangular and the frequency response  $H_{\rm E}(f)$  is sinc-shaped.
  • For system  $\rm B$,  $H_{\rm E}(f)$  is rectangular like  $G_{s}(f)$  and thus the impulse response  $h_{\rm E}(t)$  is an sinc-function.
  • Statement 3 is false:   An integrator has a rectangular impulse response and would be suitable for the realization of system  $\rm A$,  but not for system  $\rm B$.


(4)  For system  $\rm B$   ⇒   $G_{d}(f)$  nearly coincides with  $G_{s}(f)$.

  • There is only a difference in the Nyquist frequency,  but this does not affect the considerations here:
  • While  $G_{s}(f_{\rm Nyq}) = 1/2$,  $G_{d}(f_{\rm Nyq}) = 1/4$.
  • This results in a Nyquist system with rolloff factor  $r = 0$.
  • From this follows for the Nyquist frequency from the condition that the symbol duration should also be  $T = 0.5\ \rm µ s$:
$$f_{\rm 0} = f_{\rm Nyq} = \frac{1 } {2 \cdot T} = \frac{1 } {2 \cdot 0.5 \cdot 10^{-6}\,{\rm s}}\hspace{0.1cm}\underline {= 1\,{\rm MHz}}\hspace{0.05cm}.$$


(5)  For the energy of the basic transmission pulse can also be written:

$$E_{\rm B} =\int_{-\infty}^{+\infty}|G_s(f)|^2 \,{\rm d} f = G_0^2\cdot 2 f_0\hspace{0.05cm}.$$
  • Using the results from  (2)  and  (4),  it follows:
$$G_0^2 = \frac{E_{\rm B}}{2 f_0} = \frac{5 \cdot 10^{-7}\,{\rm V^2/Hz}}{2 \cdot 10^{6}\,{\rm Hz}}= 2.5 \cdot 10^{-13}\,{\rm V^2/Hz^2}\hspace{0.3cm}\Rightarrow \hspace{0.3cm}G_0 \hspace{0.1cm}\underline {= 0.5 \cdot 10^{-6}\,{\rm V/Hz}}\hspace{0.05cm}.$$


(6)  Solution 1  is correct:

  • System  $\rm A$  represents the optimal system even with peak limitation.
  • On the other hand,  system  $\rm B$  would be unsuitable due to the extremely unfavorable crest factor.