Difference between revisions of "Aufgaben:Exercise 1.6Z: Two Optimal Systems"
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− | {{quiz-Header|Buchseite= | + | {{quiz-Header|Buchseite=Digital_Signal_Transmission/Optimization_of_Baseband_Transmission_Systems |
}} | }} | ||
− | [[File:P_ID1293__Dig_Z_1_6.png|right|frame| | + | [[File:P_ID1293__Dig_Z_1_6.png|right|frame|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 N0. In both cases, the bit error probability is: | |
:pB=Q(√2⋅EB/N0). | :pB=Q(√2⋅EB/N0). | ||
− | * | + | *System $\rm A$ uses the NRZ basic transmission pulse gs(t) according to the upper sketch with amplitude s0=1 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: |
:$$G_s(f) = \left\{ \begin{array}{c} G_0 \\ | :$$G_s(f) = \left\{ \begin{array}{c} G_0 \\ | ||
0 \\ \end{array} \right.\quad | 0 \\ \end{array} \right.\quad | ||
− | \begin{array}{*{1}c} {\rm{ | + | \begin{array}{*{1}c} {\rm{for}} |
− | \\ {\rm{ | + | \\ {\rm{for}} \\ \end{array}\begin{array}{*{20}c} |
|f| < f_0 \hspace{0.05cm}, \\ | |f| < f_0 \hspace{0.05cm}, \\ | ||
|f| > f_0 \hspace{0.05cm}.\\ | |f| > f_0 \hspace{0.05cm}.\\ | ||
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− | |||
− | === | + | Notes: |
+ | *The exercise belongs to the chapter [[Digital_Signal_Transmission/Optimization_of_Baseband_Transmission_Systems|"Optimization of Baseband Transmission Systems"]]. | ||
+ | |||
+ | *Here, the pulse amplitude is given in "volts", so that the average energy per bit (EB) has the unit V2/Hz. | ||
+ | |||
+ | |||
+ | |||
+ | ===Questions=== | ||
<quiz display=simple> | <quiz display=simple> | ||
− | { | + | {At what bit rate do the two systems operate? |
|type="{}"} | |type="{}"} | ||
R = { 2 3% } Mbit/s | R = { 2 3% } Mbit/s | ||
− | { | + | {Calculate the energy per bit for system $\rm A$. |
|type="{}"} | |type="{}"} | ||
EB = { 0.5 3% } ⋅10−6 V2/Hz | EB = { 0.5 3% } ⋅10−6 V2/Hz | ||
− | { | + | {Which statements are true for the receiver filters of systems $\rm A and \rm B$? |
|type="[]"} | |type="[]"} | ||
− | + | + | +For system $\rm A$, HE(f) has a sinc-shaped curve. |
− | + | + | +For system $\rm B$, HE(f) is an ideal rectangular low-pass filter. |
− | -HE(f) | + | -HE(f) can be realized by an integrator in system $\rm B$. |
− | { | + | {For which cutoff frequency f0 does system $\rm B$ have the symbol duration T? |
|type="{}"} | |type="{}"} | ||
f0 = { 1 3% } MHz | f0 = { 1 3% } MHz | ||
− | { | + | {How large should the constant height G0 of the spectrum $\rm B be chosen so that the same energy per bit results as for system \rm A$? |
|type="{}"} | |type="{}"} | ||
G0 = { 0.5 3% } ⋅10−6 V/Hz | G0 = { 0.5 3% } ⋅10−6 V/Hz | ||
− | { | + | {Would one of the two systems be suitable even with peak limitation? |
|type="[]"} | |type="[]"} | ||
− | +System | + | +System $\rm A$, |
− | - System | + | - System $\rm B$. |
</quiz> | </quiz> | ||
− | === | + | ===Solution=== |
{{ML-Kopf}} | {{ML-Kopf}} | ||
− | '''(1)''' | + | '''(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 =2 Mbit/s_. | ||
− | '''(2)''' | + | |
+ | '''(2)''' The energy of the NRZ basic transmission pulse of system $\rm A$ is given by | ||
:$$E_{\rm B} = | :$$E_{\rm B} = | ||
\int_{-\infty}^{+\infty}g_s^2 (t)\,{\rm d} t = | \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}.$$ | s_0^2 \cdot T = {1\,{\rm V^2}}\cdot {0.5 \cdot 10^{-6}\,{\rm s}}\hspace{0.1cm}\underline { = 0.5 \cdot 10^{-6}\,{\rm V^2/Hz}}\hspace{0.05cm}.$$ | ||
− | '''(3)''' | + | |
− | *In | + | '''(3)''' The <u>first two statements are true</u>: |
− | * | + | *In both cases hE(t) must be equal in form to gs(t) and HE(f) must be equal in form to Gs(f). |
− | * | + | *Thus, for system $\rm A$, the impulse response hE(t) is rectangular and the frequency response HE(f) is sinc-shaped. |
+ | *For system $\rm B$, HE(f) is rectangular like Gs(f) and thus the impulse response hE(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)''' | + | '''(4)''' For system $\rm B$ ⇒ Gd(f) nearly coincides with Gs(f). |
+ | *There is only a difference in the Nyquist frequency, but this does not affect the considerations here: | ||
+ | *While Gs(fNyq)=1/2, Gd(fNyq)=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 $T = 0.5\ \rm µ s$: | ||
:f0=fNyq=12⋅T=12⋅0.5⋅10−6s=1MHz_. | :f0=fNyq=12⋅T=12⋅0.5⋅10−6s=1MHz_. | ||
− | + | ||
− | '''(5)''' | + | |
+ | '''(5)''' 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 | \int_{-\infty}^{+\infty}|G_s(f)|^2 \,{\rm d} f = G_0^2 | ||
\cdot 2 f_0\hspace{0.05cm}.$$ | \cdot 2 f_0\hspace{0.05cm}.$$ | ||
− | + | *Using the results from '''(2)''' and '''(4)''', it follows: | |
:$$G_0^2 = \frac{E_{\rm B}}{2 f_0} = \frac{5 \cdot 10^{-7}\,{\rm V^2/Hz}}{2 \cdot 10^{6}\,{\rm | :$$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} | Hz}}= 2.5 \cdot 10^{-13}\,{\rm V^2/Hz^2} | ||
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− | '''(6)''' | + | '''(6)''' <u>Solution 1</u> 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. |
{{ML-Fuß}} | {{ML-Fuß}} | ||
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− | [[Category: | + | [[Category:Digital Signal Transmission: Exercises|^1.4 Optimization of Baseband Systems^]] |
Latest revision as of 11:24, 4 May 2022
Consider two binary transmission systems A and B, which have the same error behavior for an AWGN channel with noise power density N0. In both cases, the bit error probability is:
- pB=Q(√2⋅EB/N0).
- System A uses the NRZ basic transmission pulse gs(t) according to the upper sketch with amplitude s0=1 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:
- The exercise belongs to the chapter "Optimization of Baseband Transmission Systems".
- 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
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.