Aufgaben:Exercise 2.12: Non-coherent Demodulation: Difference between revisions
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{{quiz-Header|Buchseite= | {{quiz-Header|Buchseite=Modulation Methods/Further AM Variants | ||
}} | }} | ||
[[File: | [[File:EN_Mod_A_2_12.png|right|frame|ASK Demodulation <br>(non-coherent) ]] | ||
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 | |||
$$ r(t) = q(t) \cdot \cos(\omega_{\rm T} \cdot t + \Delta \phi_{\rm T}) \hspace{0.05cm}.$$ | :$$ r(t) = q(t) \cdot \cos(\omega_{\rm T} \cdot t + \Delta \phi_{\rm T}) \hspace{0.05cm}.$$ | ||
The arrangement shown here allows perfect demodulation – that is: $v(t) = q(t)$ – 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: | |||
$$ z_{\rm 1, \hspace{0.08cm}E}(t) = 2 \cdot \cos(\omega_{\rm T} \cdot t) \hspace{0.05cm},$$ | :$$ z_{\rm 1, \hspace{0.08cm}E}(t) = 2 \cdot \cos(\omega_{\rm T} \cdot t) \hspace{0.05cm},$$ | ||
$$ z_{\rm 2, \hspace{0.08cm}E}(t) = -2 \cdot \sin(\omega_{\rm T} \cdot t) \hspace{0.05cm}.$$ | :$$ z_{\rm 2, \hspace{0.08cm}E}(t) = -2 \cdot \sin(\omega_{\rm T} \cdot t) \hspace{0.05cm}.$$ | ||
$ | $\rm LP_1$ 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 | |||
$$ \cos(\alpha) \cdot \cos(\beta) = | #an [[Modulation_Methods/Linear_Digital_Modulation#ASK_.E2.80.93_Amplitude_Shift_Keying|ASK signal]], | ||
$$ \sin(\alpha) \cdot \sin(\beta) = | #a [[Modulation_Methods/Linear_Digital_Modulation#BPSK_.E2.80.93_Binary_Phase_Shift_Keying|BPSK signal]]. | ||
$$ \sin(\alpha) \cdot \cos(\beta) = | |||
=== | |||
The nonlinear function $v = g(b)$ is to be determined in this exercise. | |||
Hints: | |||
*This exercise belongs to the chapter [[Modulation_Methods/Further_AM_Variants|Further AM Variants]]. | |||
*Particular reference is made to the section [[Modulation_Methods/Further_AM_Variants#Incoherent_.28non-coherent.29_Demodulation|Incoherent (non-coherent) Demodulation]]. | |||
*The following trigonometric transformations are given: | |||
:$$ \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}.$$ | |||
===Questions=== | |||
<quiz display=simple> | <quiz display=simple> | ||
{ | {What are the signals $b_1(t)$ and $b_2(t)$ in both branches – after multiplier and low-pass respectively? Which statements apply? | ||
|type="[]"} | |type="[]"} | ||
+ $b_1(t) = q(t) · cos( | + $b_1(t) = q(t) · \cos(Δϕ_{\rm T})$. | ||
- $b_2(t) = q(t) · cos( | - $b_2(t) = q(t) · \cos(Δϕ_{\rm T})$. | ||
- $b_1(t) = q(t) · sin( | - $b_1(t) = q(t) · \sin(Δϕ_{\rm T})$. | ||
+ $b_2(t) = q(t) · sin( | + $b_2(t) = q(t) · \sin(Δϕ_{\rm T})$. | ||
- $b_2(t) = q(t | - $b_1(t) = b_2(t) = q(t)$. | ||
{ | {What values of $b_{\rm min}$ and $b_{\rm max}$ does the signal $b(t)$ take on, when the unipolar source signal $q_1(t)$ is applied to the input? | ||
|type="{}"} | |type="{}"} | ||
$ | $b_{\rm min} \ = \ $ { 0. } | ||
$ | $b_{\rm max} \ = \ $ { 9 3% } | ||
{ | {How should the characteristic curve $v = g(b)$ be chosen, so that $v(t) = q(t)$ holds? | ||
|type=" | |type="()"} | ||
- $g(b) = b^2$. | - $v=g(b) = b^2$. | ||
+ $g(b) = b | + $v=g(b) = \sqrt{b}$. | ||
- $g(b) = arctan(b).$ | - $v=g(b) = \arctan(b).$ | ||
{ | {What values of $b_{\rm min}$ and $b_{\rm max}$ does the signal $b(t)$ take on, when the bipolar source signal $q_2(t)$ is applied to the input? | ||
|type="{}"} | |type="{}"} | ||
$ | $b_{\rm min} \ = \ $ { 9 3% } | ||
$ | $b_{\rm max} \ = \ $ { 9 3% } | ||
</quiz> | </quiz> | ||
=== | ===Solution=== | ||
{{ML-Kopf}} | {{ML-Kopf}} | ||
'''1 | '''(1)''' Applying the trigonometric transformations given on the exercise page and taking into account the two low-pass filters (the components around twice the carrier frequency are removed), we obtain: | ||
$$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_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}.$$ | :$$ 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}.$$ | ||
*Thus, <u>the first and fourth answers</u> are correct. | |||
'''(2)''' The sum of the squares of the two partial signals gives: | |||
:$$ 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}.$$ | |||
'''(3)''' The <u>second answer</u> is correct: | |||
:$$v=g(b) = \sqrt{b} \hspace{0.3cm} \Rightarrow \hspace{0.3cm} v(t) = \sqrt{ q^2(t) } = q(t)\hspace{0.05cm}.$$ | |||
'''(4)''' The result $b(t) = q^2(t)$ – see subtask '''(2)''' – leads here to the result: | |||
:$$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. | |||
{{ML-Fuß}} | {{ML-Fuß}} | ||
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[[Category: | [[Category:Modulation Methods: Exercises|^2.5 Other AM Variants^ ]] | ||
[[de:Aufgaben:Aufgabe 2.12: Zur nichtkohärenten Demodulation]] | |||
Latest revision as of 17:54, 16 March 2026

(non-coherent)
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 section 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) – leads here 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.