Difference between revisions of "Aufgaben:Exercise 2.3: Binary Signal and Quaternary Signal"
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− | {{quiz-Header|Buchseite= | + | {{quiz-Header|Buchseite=Digital_Signal_Transmission/Redundancy-Free_Coding |
+ | }} | ||
− | [[File:|right|]] | + | [[File:P_ID1324__Dig_A_2_3.png|right|frame|ACF and PSD of binary signal (B) and quaternary signal (Q)]] |
+ | Two redundancy-free transmission systems B and Q each with bipolar amplitude coefficients aν are to be compared. Both systems satisfy the first Nyquist condition. According to the root-root splitting, the spectrum Gd(f) of the basic detection pulse is equal in shape to the power-spectral density Φs(f) of the transmitted signal. | ||
+ | The following properties of the two systems are known: | ||
+ | *From the binary system B, the power-spectral density Φs(f) at the transmitter is known and shown in the graph together with the description parameters. | ||
− | === | + | *The quaternary system Q uses a NRZ rectangular signal with the four possible amplitude values ±s0 and ±s0/3, all with equal probability. |
+ | |||
+ | *s02 indicates the maximum instantaneous power that occurs only when one of the two "outer symbols" is transmitted. The descriptive parameters of system Q can be obtained from the triangular ACF in the adjacent graph. | ||
+ | |||
+ | |||
+ | |||
+ | |||
+ | Notes: | ||
+ | *The exercise is part of the chapter [[Digital_Signal_Transmission/Grundlagen_der_codierten_Übertragung|"Basics of Coded Transmission"]]. | ||
+ | |||
+ | *Reference is also made to the chapter [[Digital_Signal_Transmission/Redundanzfreie_Codierung|"Redundancy-Free Coding"]]. | ||
+ | |||
+ | *Consider that auto-correlation function (ACF) and power-spectral density (PSD) of a stochastic signal are always related via the Fourier transform. | ||
+ | |||
+ | |||
+ | |||
+ | |||
+ | ===Questions=== | ||
<quiz display=simple> | <quiz display=simple> | ||
− | { | + | |
+ | {What is the symbol duration T of the binary system B with Nyquist property? | ||
+ | |type="{}"} | ||
+ | T = { 5 3% } ns | ||
+ | |||
+ | |||
+ | {What is the (equivalent) bit rate RB of the binary system B ? | ||
+ | |type="{}"} | ||
+ | RB = { 200 3% } Mbit/s | ||
+ | |||
+ | |||
+ | {What is the transmitted power of the binary system B? | ||
+ | |type="{}"} | ||
+ | PS = { 200 3% } mW | ||
+ | |||
+ | {Which statements are true regarding the binary system B? | ||
|type="[]"} | |type="[]"} | ||
− | - | + | + The ACF φs(τ) of the transmitted signal is sinc2–shaped. |
− | + | + The energy ACF φ∙gs(τ) of the basic transmission pulse is sinc2–shaped. | |
+ | - The basic transmission pulse gs(t) itself is sinc2–shaped. | ||
+ | |||
+ | {What is the symbol duration T of the quaternary system Q? | ||
+ | |type="{}"} | ||
+ | T = { 10 3% } ns | ||
− | { | + | {What is the equivalent bit rate RB of the quaternary system Q? |
|type="{}"} | |type="{}"} | ||
− | $\ | + | $R_{\rm B} \ = \ $ { 200 3% } Mbit/s |
+ | {What is the transmitted power PS of the quaternary system Q? | ||
+ | |type="{}"} | ||
+ | PS = { 100 3% } mW | ||
+ | |||
+ | |||
+ | {What is the maximum instantaneous transmitted power of the quaternary system Q? | ||
+ | |type="{}"} | ||
+ | s02 = { 180 3% } mW | ||
</quiz> | </quiz> | ||
− | === | + | ===Solution=== |
{{ML-Kopf}} | {{ML-Kopf}} | ||
− | '''(1)''' | + | '''(1)''' The Nyquist frequency fNyq=100 MHz can be read from the diagram. From this follows according to the properties of Nyquist systems: |
− | '''(2)''' | + | :fNyq=12⋅T⇒T=12⋅fNyq=5ns_. |
− | '''(3)''' | + | |
− | '''(4)''' | + | |
− | '''(5)''' | + | '''(2)''' In the binary system, the bit rate is also the information flow and it holds: |
− | '''(6)''' | + | :RB=1/T=200Mbit/s_=2⋅fNyq⋅bit/Hz. |
+ | |||
+ | |||
+ | '''(3)''' The transmitted power is equal to the integral over Φs(f) and can be calculated as a triangular area: | ||
+ | :PS= ∫+∞−∞Φs(f)df=10−9WHz⋅200MHz=200mW_. | ||
+ | |||
+ | |||
+ | '''(4)''' The <u>first two statements</u> are correct: | ||
+ | *The Fourier inverse transform of the power-spectral density Φs(f) gives the sinc2–shaped ACF φs(τ). In general, the following relationship also holds: | ||
+ | :φs(τ)=+∞∑λ=−∞1/T⋅φa(λ)⋅φ∙gs(τ−λ⋅T). | ||
+ | *However, for a redundancy-free binary system, φa(λ=0)=1, while all other discrete ACF values φa(λ≠0) are equal to 0. Thus, the energy ACF also has a sinc2–shaped curve (note: energy ACF and energy PSD are each dotted in this tutorial): | ||
+ | :φ∙gs(τ)=T⋅φs(τ). | ||
+ | *The last statement is not true. For the following reasoning, we assume for simplicity that gs(t) is symmetric and thus Gs(f) is real. Then holds: | ||
+ | :Φs(f)=1/T⋅|Gs(f)|2⇒Gs(f)=√T⋅Φs(f)∙−−−∘gs(t). | ||
+ | *Due to the square root in the above equation, the basic transmission pulse gs(t) is not sinc2–shaped in contrast to the basic detection pulse gd(t), which is equal in shape to the energy ACF φ∙gs(τ) and thus sinc2–shaped. At the same time, \varphi^{^{\bullet}}_{gs}(\tau) = g_{s}(\tau) ∗ g_{s}(–\tau) holds. | ||
+ | |||
+ | |||
+ | |||
+ | '''(5)''' The ACF \varphi_{s}(\tau) is limited to the range |\tau| ≤ T when the basic transmission pulse is an NRZ rectangle. From the graph, the symbol duration T \underline{= 10 \ \rm ns}. | ||
+ | |||
+ | |||
+ | '''(6)''' For the quaternary signal, the information flow is the same as for the binary signal above because of the double symbol duration: | ||
+ | :R_{\rm B} = {{\rm log_2(4)} }/ { T} \hspace{0.15cm}\underline {= 200\,\,{\rm Mbit/s}}\hspace{0.05cm}. | ||
+ | |||
+ | |||
+ | '''(7)''' The transmitted power is equal to the ACF value at \tau = 0 and can be read from the graph: | ||
+ | :P_{\rm S} = \hspace{0.15cm}\underline {100\,\,{\rm mW}}. | ||
+ | |||
+ | |||
+ | '''(8)''' For the redundancy-free quaternary signal with NRZ rectangular pulses, the average transmitted power is: | ||
+ | :P_{\rm S} = {1}/ { 4} \cdot \left [ (-s_0)^2 + (-s_0/3)^2 + (+s_0/3)^2 +(+s_0)^2 \right ] = {5}/ { 9} \cdot s_0^2 | ||
+ | :\Rightarrow \hspace{0.3cm}s_0^2 = {9}/ {5} \cdot P_{\rm S} = {9}/ {5} \cdot 100\,\,{\rm mW}\hspace{0.15cm}\underline { = 180\,\,{\rm mW}}\hspace{0.05cm}. | ||
{{ML-Fuß}} | {{ML-Fuß}} | ||
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− | [[Category: | + | [[Category:Digital Signal Transmission: Exercises|^2.2 Redundancy-Free Coding^]] |
Latest revision as of 17:16, 3 June 2022
Two redundancy-free transmission systems \rm B and \rm Q each with bipolar amplitude coefficients a_{\nu} are to be compared. Both systems satisfy the first Nyquist condition. According to the root-root splitting, the spectrum G_{d}(f) of the basic detection pulse is equal in shape to the power-spectral density {\it \Phi}_{s}(f) of the transmitted signal.
The following properties of the two systems are known:
- From the binary system \rm B, the power-spectral density {\it \Phi}_{s}(f) at the transmitter is known and shown in the graph together with the description parameters.
- The quaternary system \rm Q uses a NRZ rectangular signal with the four possible amplitude values ±s_{0} and ±s_{0}/3, all with equal probability.
- {s_{0}}^{2} indicates the maximum instantaneous power that occurs only when one of the two "outer symbols" is transmitted. The descriptive parameters of system \rm Q can be obtained from the triangular ACF in the adjacent graph.
Notes:
- The exercise is part of the chapter "Basics of Coded Transmission".
- Reference is also made to the chapter "Redundancy-Free Coding".
- Consider that auto-correlation function \rm (ACF) and power-spectral density \rm (PSD) of a stochastic signal are always related via the Fourier transform.
Questions
Solution
- f_{\rm Nyq} = \frac{1 } {2 \cdot T} \hspace{0.3cm}\Rightarrow \hspace{0.3cm} T = \frac{1 } {2 \cdot f_{\rm Nyq}} \hspace{0.15cm}\underline{ =5\,{\rm ns}}\hspace{0.05cm}.
(2) In the binary system, the bit rate is also the information flow and it holds:
- R_{\rm B} = {1 }/ { T} \hspace{0.15cm}\underline {= 200\,{\rm Mbit/s}}= 2 \cdot f_{\rm Nyq} \cdot{\rm bit}/{\rm Hz}\hspace{0.05cm}.
(3) The transmitted power is equal to the integral over {\it \Phi}_{s}(f) and can be calculated as a triangular area:
- P_{\rm S} = \ \int_{-\infty}^{+\infty} {\it \Phi}_s(f) \,{\rm d} f = 10^{-9} \frac{\rm W}{\rm Hz} \cdot 200\,\,{\rm MHz} \hspace{0.15cm}\underline { = 200\,\,{\rm mW}}.
(4) The first two statements are correct:
- The Fourier inverse transform of the power-spectral density {\it \Phi}_{s}(f) gives the \rm sinc^{2}–shaped ACF \varphi_{s}(\tau). In general, the following relationship also holds:
- \varphi_s(\tau) = \sum_{\lambda = -\infty}^{+\infty}{1}/{T} \cdot \varphi_a(\lambda)\cdot \varphi^{^{\bullet}}_{gs}(\tau - \lambda \cdot T)\hspace{0.05cm}.
- However, for a redundancy-free binary system, \varphi_{a}(\lambda = 0) = 1, while all other discrete ACF values \varphi_{a}(\lambda \neq 0) are equal to 0. Thus, the energy ACF also has a \rm sinc^{2}–shaped curve (note: energy ACF and energy PSD are each dotted in this tutorial):
- \varphi^{^{\bullet}}_{gs}(\tau ) = T \cdot \varphi_s(\tau) \hspace{0.05cm}.
- The last statement is not true. For the following reasoning, we assume for simplicity that g_{s}(t) is symmetric and thus G_{s}(f) is real. Then holds:
- {\it \Phi}_{s}(f) = {1 }/ { T} \cdot |G_s(f)|^2\hspace{0.3cm}\Rightarrow \hspace{0.3cm}G_s(f) = \sqrt{{ T} \cdot {\it \Phi}_{s}(f)}\hspace{0.4cm} \bullet\!\!-\!\!\!-\!\!\!-\!\!\circ \hspace{0.4cm}g_s(t) \hspace{0.05cm}.
- Due to the square root in the above equation, the basic transmission pulse g_{s}(t) is not \rm sinc^{2}–shaped in contrast to the basic detection pulse g_{d}(t), which is equal in shape to the energy ACF \varphi^{^{\bullet}}_{gs}(\tau) and thus \rm sinc^{2}–shaped. At the same time, \varphi^{^{\bullet}}_{gs}(\tau) = g_{s}(\tau) ∗ g_{s}(–\tau) holds.
(5) The ACF \varphi_{s}(\tau) is limited to the range |\tau| ≤ T when the basic transmission pulse is an NRZ rectangle. From the graph, the symbol duration T \underline{= 10 \ \rm ns}.
(6) For the quaternary signal, the information flow is the same as for the binary signal above because of the double symbol duration:
- R_{\rm B} = {{\rm log_2(4)} }/ { T} \hspace{0.15cm}\underline {= 200\,\,{\rm Mbit/s}}\hspace{0.05cm}.
(7) The transmitted power is equal to the ACF value at \tau = 0 and can be read from the graph:
- P_{\rm S} = \hspace{0.15cm}\underline {100\,\,{\rm mW}}.
(8) For the redundancy-free quaternary signal with NRZ rectangular pulses, the average transmitted power is:
- P_{\rm S} = {1}/ { 4} \cdot \left [ (-s_0)^2 + (-s_0/3)^2 + (+s_0/3)^2 +(+s_0)^2 \right ] = {5}/ { 9} \cdot s_0^2
- \Rightarrow \hspace{0.3cm}s_0^2 = {9}/ {5} \cdot P_{\rm S} = {9}/ {5} \cdot 100\,\,{\rm mW}\hspace{0.15cm}\underline { = 180\,\,{\rm mW}}\hspace{0.05cm}.