Difference between revisions of "Aufgaben:Exercise 2.12: Non-coherent Demodulation"
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Consider an amplitude modulated signal: | Consider an amplitude modulated signal: | ||
:$$ s(t) = q(t) \cdot \cos(\omega_{\rm T} \cdot t) \hspace{0.05cm}.$$ | :$$ s(t) = q(t) \cdot \cos(\omega_{\rm T} \cdot t) \hspace{0.05cm}.$$ | ||
− | Reaching the receiver based on the channel propagation time, the signal is | + | Reaching the receiver based on the channel propagation time, the signal is |
:$$ r(t) = q(t) \cdot \cos(\omega_{\rm T} \cdot t + \Delta \phi_{\rm T}) \hspace{0.05cm}.$$ | :$$ r(t) = q(t) \cdot \cos(\omega_{\rm T} \cdot t + \Delta \phi_{\rm T}) \hspace{0.05cm}.$$ | ||
− | The arrangement shown here allows perfect demodulation – that is | + | The arrangement shown here allows perfect demodulation – that is: $v(t) = q(t)$ – without knowledge of the phase $Δϕ_T$, but only if the source signal $q(t)$ satisfies certain conditions. |
The two receiver-side carrier signals are: | The two receiver-side carrier signals are: | ||
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:$$ z_{\rm 2, \hspace{0.08cm}E}(t) = -2 \cdot \sin(\omega_{\rm T} \cdot t) \hspace{0.05cm}.$$ | :$$ z_{\rm 2, \hspace{0.08cm}E}(t) = -2 \cdot \sin(\omega_{\rm T} \cdot t) \hspace{0.05cm}.$$ | ||
− | $\rm | + | $\rm LP_1$ and $\rm LP_2$ denote two ideal (rectangular) low-pass filters, each with cutoff frequency equal to the carrier frequency $f_{\rm T}$. |
− | + | We consider as (digital) source signals: | |
− | + | # the unipolar square wave signal $q_1(t)$ with dimensionless amplitude values $0$ and $3$, | |
− | + | # the bipolar square wave signal $q_2(t)$ with the dimensionless amplitude values $±3$. | |
− | With respect to $s(t)$ | + | With respect to $s(t)$, these two signals result in |
+ | #an [[Modulation_Methods/Linear_Digital_Modulation#ASK_.E2.80.93_Amplitude_Shift_Keying|ASK signal]], | ||
+ | #a [[Modulation_Methods/Linear_Digital_Modulation#BPSK_.E2.80.93_Binary_Phase_Shift_Keying|BPSK signal]]. | ||
+ | |||
The nonlinear function $v = g(b)$ is to be determined in this exercise. | The nonlinear function $v = g(b)$ is to be determined in this exercise. | ||
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− | + | Hints: | |
− | + | *This exercise belongs to the chapter [[Modulation_Methods/Further_AM_Variants|Further AM Variants]]. | |
− | |||
− | |||
− | |||
− | *This exercise belongs to the chapter [[Modulation_Methods/Further_AM_Variants|Further AM Variants]]. | ||
*Particular reference is made to the page [[Modulation_Methods/Further_AM_Variants#Incoherent_.28non-coherent.29_Demodulation|Incoherent (non-coherent) Demodulation]]. | *Particular reference is made to the page [[Modulation_Methods/Further_AM_Variants#Incoherent_.28non-coherent.29_Demodulation|Incoherent (non-coherent) Demodulation]]. | ||
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<quiz display=simple> | <quiz display=simple> | ||
− | {What are the signals $b_1(t)$ and $b_2(t)$ in both branches – after multiplier and | + | {What are the signals $b_1(t)$ and $b_2(t)$ in both branches – after multiplier and low-pass respectively? Which statements apply? |
|type="[]"} | |type="[]"} | ||
+ $b_1(t) = q(t) · \cos(Δϕ_{\rm T})$. | + $b_1(t) = q(t) · \cos(Δϕ_{\rm T})$. | ||
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- $b_1(t) = b_2(t) = q(t)$. | - $b_1(t) = b_2(t) = q(t)$. | ||
− | {What values of $b_{\rm min}$ and $b_{\rm max}$ does the signal $b(t)$ take on, when the unipolar source signal $q_1(t)$ is applied to the input? | + | {What values of $b_{\rm min}$ and $b_{\rm max}$ does the signal $b(t)$ take on, when the unipolar source signal $q_1(t)$ is applied to the input? |
|type="{}"} | |type="{}"} | ||
$b_{\rm min} \ = \ $ { 0. } | $b_{\rm min} \ = \ $ { 0. } | ||
$b_{\rm max} \ = \ $ { 9 3% } | $b_{\rm max} \ = \ $ { 9 3% } | ||
− | {How should the characteristic curve $v = g(b)$ be chosen, so that $v(t) = q(t)$ holds? | + | {How should the characteristic curve $v = g(b)$ be chosen, so that $v(t) = q(t)$ holds? |
|type="()"} | |type="()"} | ||
- $v=g(b) = b^2$. | - $v=g(b) = b^2$. | ||
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− | {What values of $b_{\rm min}$ and $b_{\rm max}$ does the signal $b(t)$ take on, when the bipolar source signal $q_2(t)$ is applied to the input? | + | {What values of $b_{\rm min}$ and $b_{\rm max}$ does the signal $b(t)$ take on, when the bipolar source signal $q_2(t)$ is applied to the input? |
|type="{}"} | |type="{}"} | ||
$b_{\rm min} \ = \ $ { 9 3% } | $b_{\rm min} \ = \ $ { 9 3% } |
Revision as of 17:07, 18 February 2022
Consider an amplitude modulated signal:
- $$ s(t) = q(t) \cdot \cos(\omega_{\rm T} \cdot t) \hspace{0.05cm}.$$
Reaching the receiver based on the channel propagation time, the signal is
- $$ r(t) = q(t) \cdot \cos(\omega_{\rm T} \cdot t + \Delta \phi_{\rm T}) \hspace{0.05cm}.$$
The arrangement shown here allows perfect demodulation – that is: $v(t) = q(t)$ – without knowledge of the phase $Δϕ_T$, but only if the source signal $q(t)$ satisfies certain conditions.
The two receiver-side carrier signals are:
- $$ z_{\rm 1, \hspace{0.08cm}E}(t) = 2 \cdot \cos(\omega_{\rm T} \cdot t) \hspace{0.05cm},$$
- $$ z_{\rm 2, \hspace{0.08cm}E}(t) = -2 \cdot \sin(\omega_{\rm T} \cdot t) \hspace{0.05cm}.$$
$\rm LP_1$ and $\rm LP_2$ denote two ideal (rectangular) low-pass filters, each with cutoff frequency equal to the carrier frequency $f_{\rm T}$.
We consider as (digital) source signals:
- the unipolar square wave signal $q_1(t)$ with dimensionless amplitude values $0$ and $3$,
- the bipolar square wave signal $q_2(t)$ with the dimensionless amplitude values $±3$.
With respect to $s(t)$, these two signals result in
- an ASK signal,
- a BPSK signal.
The nonlinear function $v = g(b)$ is to be determined in this exercise.
Hints:
- This exercise belongs to the chapter Further AM Variants.
- Particular reference is made to the page Incoherent (non-coherent) Demodulation.
- The following trigonometric transformations are given:
- $$ \cos(\alpha) \cdot \cos(\beta) = 1/2 \cdot \big[ \cos(\alpha - \beta)+ \cos(\alpha + \beta) \big],$$
- $$ \sin(\alpha) \cdot \sin(\beta) = 1/2 \cdot \big[ \cos(\alpha - \beta)- \cos(\alpha + \beta) \big],$$
- $$ \sin(\alpha) \cdot \cos(\beta) = 1/2 \cdot \big[ \sin(\alpha - \beta)+ \sin(\alpha + \beta) \big] \hspace{0.05cm}.$$
Questions
Solution
- $$b_1(t) = q(t) \cdot \cos(\omega_{\rm T} \cdot t + \Delta \phi_{\rm T}) \cdot 2 \cdot \cos(\omega_{\rm T} \cdot t) = q(t) \cdot \cos(\Delta \phi_{\rm T})\hspace{0.05cm},$$
- $$ b_2(t) = q(t) \cdot \cos(\omega_{\rm T} \cdot t + \Delta \phi_{\rm T}) \cdot (-2) \cdot \sin(\omega_{\rm T} \cdot t) = q(t) \cdot \sin(\Delta \phi_{\rm T})\hspace{0.05cm}.$$
- Thus, the first and fourth answers are correct.
(2) The sum of the squares of the two partial signals gives:
- $$ b(t) = b_1^2(t) + b_2^2(t)= q^2(t) \cdot \left( \cos^2(\Delta \phi_{\rm T})+ \sin^2(\Delta \phi_{\rm T})\right) = q^2(t)\hspace{0.05cm}.$$
The possible amplitude values are thus:
- $$b_{\rm min}\hspace{0.15cm}\underline{ = 0},$$
- $$ b_{\rm max}\hspace{0.15cm}\underline{ =9}.$$
(3) The second answer is correct:
- $$v=g(b) = \sqrt{b} \hspace{0.3cm} \Rightarrow \hspace{0.3cm} v(t) = \sqrt{ q^2(t) } = q(t)\hspace{0.05cm}.$$
(4) The result $b(t) = q^2(t)$ – see subtask (2) – here leads to the result:
- $$b_{\rm min}\hspace{0.15cm}\underline{ = 9},$$
- $$b_{\rm max}\hspace{0.15cm}\underline{ =9}.$$
This shows that the demodulator considered here only functions, if at all times $q(t) ≥ 0$ or , $q(t) ≤ 0$ holds, and this is known at the receiver.